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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812780</id>
		<title>MRD:01541238</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812780"/>
		<updated>2020-06-04T19:25:46Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 10. Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= The Molecular reaction dynamics computational lab report =&lt;br /&gt;
&lt;br /&gt;
=== Question 1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
[[File:1.png]][[File:2.png]]&lt;br /&gt;
&lt;br /&gt;
These two diagrams are the counter plot and skew plot from a three H atoms model. A H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system.&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface diagram (gallery 2). The black reaction trajectory line shows the minimum energy path of the reactants to the products.&lt;br /&gt;
&lt;br /&gt;
When the trajectory line pass through the transition structure it shows a wavy line. And the transition state is defined as the maximum on the black trajectory minimum energy path.&lt;br /&gt;
&lt;br /&gt;
Mathematically the transition state point has the special property that ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 and the energy is higher than any other local minimum points on the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
And the transition state point is a critical point which can be identified by secondary derivative =0. The difference between local minimum is that they have a non zero second derivative number.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok but be careful with respect to what you mean by secondary derivative. You are looking for the secondary partial derivative of the reaction co ordinate with respect to the energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:49, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. ===&lt;br /&gt;
My best estimate of the transition state position &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;&#039;&#039;&#039;= 90.8 pm and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
According to the theory, when the structure is at transition structure, the trajectory point will only oscillate at on point.&lt;br /&gt;
&lt;br /&gt;
[[File:Dist vs time2.png]]&lt;br /&gt;
&lt;br /&gt;
The diagram above is the &#039;internuclear distance vs time&#039; plot for my best estimation of the positions. As shown on the diagram, there is almost no oscillation of the bond distances between B-C and A-B which means&lt;br /&gt;
&lt;br /&gt;
the structure is under a &#039;stable&#039; state and this structure is called transition state structure.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what did you use to approximate this value or get closer to it?  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:53, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 3. Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ. ===&lt;br /&gt;
In my case, positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;91.8&#039;&#039;&#039; pm,  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;90.8 &#039;&#039;&#039;pm and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the new trajectory calculated.&lt;br /&gt;
&lt;br /&gt;
[[File:6_01541238.png]][[File:4_2_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Compare with two diagrams, the MEP doesn&#039;t have the vibrations of the atoms during the process while the trajectory shows oscillation to the products. And other remains the same, both direct to the same product.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, how do the calculation methods differ? The MEP resets the momentum to 0 with each step.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:57, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 4. Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ===&lt;br /&gt;
For the initial positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 74 pm and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 200 pm&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
7_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|unreactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
8_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Don&#039;t have enough energy to overcome the activation barrier, bounce&lt;br /&gt;
back to the more energy preferred state.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
9_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
10_2_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is much higher than the previous ones. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
twice and back to the initial conditions.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
11_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is higher than the previous one. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
three times and complete the reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You could have described the trajectories with slightly more detail.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The table above list some occasions for the different initial energies for the system. The table shows the energy is critically controlled in order to make the reaction complete.&lt;br /&gt;
&lt;br /&gt;
The total energy can&#039;t be too low so that can&#039;t pass though the energy barrier or too high to bounce back even through the transition state point twice.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, what energy prevents the stable formation of the products? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 5. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
With compare with experimental values, the Transition State Theory predictions will be over-estimated. Transition State Theory assumes the transition state structure will not go back to the initial reactants since the transition &lt;br /&gt;
&lt;br /&gt;
structure is formed. An equilibrium will form between the reactants and the transition states. However, in real life there is barrier recrossing cause the transition state structure goes back.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful what you mean by &#039;real life&#039;, do you mean in reference the modelled system or an actual reaction? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Moreover, the Transition State Theory is treated classically Quantum mechanical effect like tunnelling effect is ignored. In real situations, particles with lower kinetic energy might able to cross the high energy barrier caused &lt;br /&gt;
&lt;br /&gt;
by tunnelling effect. Transition State Theory may overestimate the rate because it requires more energy to overcome the barrier.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You are correct that TST will overestimate the rate, but how do th results in the table relate to TST? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 6. By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?  ===&lt;br /&gt;
[[File:12_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
As shown in the diagram above, it is a potential energy surfaces for F + H2 system. The LHS is for HF energy level which is lower than H2 energy level on the RHS. Because the F-H bond is stronger than H-H bond for &lt;br /&gt;
&lt;br /&gt;
F + H2 reaction is endothermic as stronger F-H bond formation required energy. Vice Versa, H + HF reaction is exothermic for strong H-F bond is broke.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| I tihnk you may have misinterpeted the PES here. F + H2 is an exothermic reaction. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:10, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 7. Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
[[File:13_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Diagram above is the &#039;internuclear distance vs time&#039; for my estimated transition state structure.&lt;br /&gt;
&lt;br /&gt;
My best estimated transition state positions are F-H = 180.8 pm and H-H = 74.5 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, you need to make it clear how you calculated this or what you did to get closer to your answer. This answer is correct though, well done for including th einternuclear vs time. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 8. Report the activation energy for both reactions. ===&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;reaction, the activation energy is the energy differences between reactant and transition state structure. &lt;br /&gt;
&lt;br /&gt;
Ea=1.075 kJ/mol&lt;br /&gt;
&lt;br /&gt;
For H + HF reaction,&lt;br /&gt;
&lt;br /&gt;
Ea=126.682 kJ/mol&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Similar to the previous comment, you need to make it clear how you determined the energy of the TS and reactant / product. You could have included an energy vs time plot to show this.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:14, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 9. In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
[[File:14_01541238.png]][[File:15_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:16_01541238.png]][[File:17_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
For the F + H2 reaction. It is an exothermic reaction as the strong F-H bond formed. The potential energy will transfer to kinetic energy in order to complete the reaction. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|This contradicts your last statement. Be careful with your classification. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:21, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
On diagram 1, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It shows that F-H bond is formed then break apart. Potential energy is transferred to kinetic energy that cause the recrossing &lt;br /&gt;
&lt;br /&gt;
barrier and go back to initial structure as the kinetic energy is too large. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|What does diagram 1 refer to? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:21, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
On diagram 2, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The diagram clearly shows 0.526 kJ kinetic energy is transferred which is lower than Activation energy and the reaction can&#039;t&lt;br /&gt;
&lt;br /&gt;
happen. F-H bond not formed.&lt;br /&gt;
&lt;br /&gt;
On diagram 3, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. F-H bond is formed after several formation and breakage. A significant amount of potential energy transfer into kinetic energy &lt;br /&gt;
&lt;br /&gt;
cause the oscillation for the middle H atom during the reaction.&lt;br /&gt;
&lt;br /&gt;
On diagram 4, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.6 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Kinetic energy is 1.707 kJ/mol overcomes the activation barrier and from the F-H bond.&lt;br /&gt;
&lt;br /&gt;
[[File:18_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
On the reverse reaction H + HF, the initial set is H-H = 230 pm and H-F = 100 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -20 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This diagram is one possible reactive trajectory for the reaction to complete. H atom carries 380.526 kJ/mol&lt;br /&gt;
&lt;br /&gt;
to collide with H-F molecule and form new H-H bond.&lt;br /&gt;
&lt;br /&gt;
In conclusion, the kinetic energy can be expressed as temperature. As the potential energy is transferred into kinetic energy, temperature will raise as the result of kinetic energy increases. Monitoring the temperature can help us&lt;br /&gt;
&lt;br /&gt;
to confirm this mechanism processes.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You are correct but by what mechanism does the temperature raise and what temperature is raising? Calorimetry allows us to detect temperature, perhaps you could hve explained one of these methods. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:21, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 10. Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
Translational energy is due to the change in positions and states while vibrational energy is due to the change in structure of molecules. In fact, the translation energy is more effective in promoting reactions for system with early&lt;br /&gt;
&lt;br /&gt;
barrier, whereas vibrational energy is more effective for reactions with late barrier. The position of the transition state is at the top of the activation energy barrier curve on a energy-process diagram. As a result, if the transition state&lt;br /&gt;
&lt;br /&gt;
structure is similar to reactant (early barrier) translational energy is more effective. Vice Versa, if the transition state structure is more similar to the product (late barrier) vibrational energy is more effective. Moreover, symmetric &lt;br /&gt;
&lt;br /&gt;
structure always have higher reaction rate and reactivity than unsymmetric structure.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|How does an exo/endothermic reaction relate to Hammonds postulate and Polanyis rules? You may have been able to further explore this question with reference to the system you were studying which shows exo and endothermicity depending on the reaction direction. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:25, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Your report may have been imrpoved with references, such as one to Polanyis rules. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:25, 4 June 2020 (BST)}}&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812779</id>
		<title>MRD:01541238</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812779"/>
		<updated>2020-06-04T19:21:52Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 9. In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= The Molecular reaction dynamics computational lab report =&lt;br /&gt;
&lt;br /&gt;
=== Question 1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
[[File:1.png]][[File:2.png]]&lt;br /&gt;
&lt;br /&gt;
These two diagrams are the counter plot and skew plot from a three H atoms model. A H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system.&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface diagram (gallery 2). The black reaction trajectory line shows the minimum energy path of the reactants to the products.&lt;br /&gt;
&lt;br /&gt;
When the trajectory line pass through the transition structure it shows a wavy line. And the transition state is defined as the maximum on the black trajectory minimum energy path.&lt;br /&gt;
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Mathematically the transition state point has the special property that ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 and the energy is higher than any other local minimum points on the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
And the transition state point is a critical point which can be identified by secondary derivative =0. The difference between local minimum is that they have a non zero second derivative number.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok but be careful with respect to what you mean by secondary derivative. You are looking for the secondary partial derivative of the reaction co ordinate with respect to the energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:49, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. ===&lt;br /&gt;
My best estimate of the transition state position &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;&#039;&#039;&#039;= 90.8 pm and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
According to the theory, when the structure is at transition structure, the trajectory point will only oscillate at on point.&lt;br /&gt;
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[[File:Dist vs time2.png]]&lt;br /&gt;
&lt;br /&gt;
The diagram above is the &#039;internuclear distance vs time&#039; plot for my best estimation of the positions. As shown on the diagram, there is almost no oscillation of the bond distances between B-C and A-B which means&lt;br /&gt;
&lt;br /&gt;
the structure is under a &#039;stable&#039; state and this structure is called transition state structure.&lt;br /&gt;
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{{fontcolor1|green|Ok, what did you use to approximate this value or get closer to it?  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:53, 4 June 2020 (BST)}}&lt;br /&gt;
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=== Question 3. Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ. ===&lt;br /&gt;
In my case, positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;91.8&#039;&#039;&#039; pm,  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;90.8 &#039;&#039;&#039;pm and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the new trajectory calculated.&lt;br /&gt;
&lt;br /&gt;
[[File:6_01541238.png]][[File:4_2_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Compare with two diagrams, the MEP doesn&#039;t have the vibrations of the atoms during the process while the trajectory shows oscillation to the products. And other remains the same, both direct to the same product.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, how do the calculation methods differ? The MEP resets the momentum to 0 with each step.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:57, 4 June 2020 (BST)}}&lt;br /&gt;
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=== Question 4. Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ===&lt;br /&gt;
For the initial positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 74 pm and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 200 pm&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
7_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|unreactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
8_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Don&#039;t have enough energy to overcome the activation barrier, bounce&lt;br /&gt;
back to the more energy preferred state.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
9_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
10_2_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is much higher than the previous ones. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
twice and back to the initial conditions.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
11_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is higher than the previous one. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
three times and complete the reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You could have described the trajectories with slightly more detail.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The table above list some occasions for the different initial energies for the system. The table shows the energy is critically controlled in order to make the reaction complete.&lt;br /&gt;
&lt;br /&gt;
The total energy can&#039;t be too low so that can&#039;t pass though the energy barrier or too high to bounce back even through the transition state point twice.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, what energy prevents the stable formation of the products? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
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=== Question 5. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
With compare with experimental values, the Transition State Theory predictions will be over-estimated. Transition State Theory assumes the transition state structure will not go back to the initial reactants since the transition &lt;br /&gt;
&lt;br /&gt;
structure is formed. An equilibrium will form between the reactants and the transition states. However, in real life there is barrier recrossing cause the transition state structure goes back.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful what you mean by &#039;real life&#039;, do you mean in reference the modelled system or an actual reaction? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Moreover, the Transition State Theory is treated classically Quantum mechanical effect like tunnelling effect is ignored. In real situations, particles with lower kinetic energy might able to cross the high energy barrier caused &lt;br /&gt;
&lt;br /&gt;
by tunnelling effect. Transition State Theory may overestimate the rate because it requires more energy to overcome the barrier.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You are correct that TST will overestimate the rate, but how do th results in the table relate to TST? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 6. By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?  ===&lt;br /&gt;
[[File:12_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
As shown in the diagram above, it is a potential energy surfaces for F + H2 system. The LHS is for HF energy level which is lower than H2 energy level on the RHS. Because the F-H bond is stronger than H-H bond for &lt;br /&gt;
&lt;br /&gt;
F + H2 reaction is endothermic as stronger F-H bond formation required energy. Vice Versa, H + HF reaction is exothermic for strong H-F bond is broke.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| I tihnk you may have misinterpeted the PES here. F + H2 is an exothermic reaction. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:10, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 7. Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
[[File:13_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Diagram above is the &#039;internuclear distance vs time&#039; for my estimated transition state structure.&lt;br /&gt;
&lt;br /&gt;
My best estimated transition state positions are F-H = 180.8 pm and H-H = 74.5 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, you need to make it clear how you calculated this or what you did to get closer to your answer. This answer is correct though, well done for including th einternuclear vs time. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 8. Report the activation energy for both reactions. ===&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;reaction, the activation energy is the energy differences between reactant and transition state structure. &lt;br /&gt;
&lt;br /&gt;
Ea=1.075 kJ/mol&lt;br /&gt;
&lt;br /&gt;
For H + HF reaction,&lt;br /&gt;
&lt;br /&gt;
Ea=126.682 kJ/mol&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Similar to the previous comment, you need to make it clear how you determined the energy of the TS and reactant / product. You could have included an energy vs time plot to show this.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:14, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 9. In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
[[File:14_01541238.png]][[File:15_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:16_01541238.png]][[File:17_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
For the F + H2 reaction. It is an exothermic reaction as the strong F-H bond formed. The potential energy will transfer to kinetic energy in order to complete the reaction. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|This contradicts your last statement. Be careful with your classification. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:21, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
On diagram 1, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It shows that F-H bond is formed then break apart. Potential energy is transferred to kinetic energy that cause the recrossing &lt;br /&gt;
&lt;br /&gt;
barrier and go back to initial structure as the kinetic energy is too large. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|What does diagram 1 refer to? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:21, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
On diagram 2, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The diagram clearly shows 0.526 kJ kinetic energy is transferred which is lower than Activation energy and the reaction can&#039;t&lt;br /&gt;
&lt;br /&gt;
happen. F-H bond not formed.&lt;br /&gt;
&lt;br /&gt;
On diagram 3, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. F-H bond is formed after several formation and breakage. A significant amount of potential energy transfer into kinetic energy &lt;br /&gt;
&lt;br /&gt;
cause the oscillation for the middle H atom during the reaction.&lt;br /&gt;
&lt;br /&gt;
On diagram 4, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.6 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Kinetic energy is 1.707 kJ/mol overcomes the activation barrier and from the F-H bond.&lt;br /&gt;
&lt;br /&gt;
[[File:18_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
On the reverse reaction H + HF, the initial set is H-H = 230 pm and H-F = 100 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -20 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This diagram is one possible reactive trajectory for the reaction to complete. H atom carries 380.526 kJ/mol&lt;br /&gt;
&lt;br /&gt;
to collide with H-F molecule and form new H-H bond.&lt;br /&gt;
&lt;br /&gt;
In conclusion, the kinetic energy can be expressed as temperature. As the potential energy is transferred into kinetic energy, temperature will raise as the result of kinetic energy increases. Monitoring the temperature can help us&lt;br /&gt;
&lt;br /&gt;
to confirm this mechanism processes.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You are correct but by what mechanism does the temperature raise and what temperature is raising? Calorimetry allows us to detect temperature, perhaps you could hve explained one of these methods. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:21, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 10. Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
Translational energy is due to the change in positions and states while vibrational energy is due to the change in structure of molecules. In fact, the translation energy is more effective in promoting reactions for system with early&lt;br /&gt;
&lt;br /&gt;
barrier, whereas vibrational energy is more effective for reactions with late barrier. The position of the transition state is at the top of the activation energy barrier curve on a energy-process diagram. As a result, if the transition state&lt;br /&gt;
&lt;br /&gt;
structure is similar to reactant (early barrier) translational energy is more effective. Vice Versa, if the transition state structure is more similar to the product (late barrier) vibrational energy is more effective. Moreover, symmetric &lt;br /&gt;
&lt;br /&gt;
structure always have higher reaction rate and reactivity than unsymmetric structure.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812778</id>
		<title>MRD:01541238</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812778"/>
		<updated>2020-06-04T19:14:19Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 8. Report the activation energy for both reactions. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= The Molecular reaction dynamics computational lab report =&lt;br /&gt;
&lt;br /&gt;
=== Question 1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
[[File:1.png]][[File:2.png]]&lt;br /&gt;
&lt;br /&gt;
These two diagrams are the counter plot and skew plot from a three H atoms model. A H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system.&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface diagram (gallery 2). The black reaction trajectory line shows the minimum energy path of the reactants to the products.&lt;br /&gt;
&lt;br /&gt;
When the trajectory line pass through the transition structure it shows a wavy line. And the transition state is defined as the maximum on the black trajectory minimum energy path.&lt;br /&gt;
&lt;br /&gt;
Mathematically the transition state point has the special property that ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 and the energy is higher than any other local minimum points on the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
And the transition state point is a critical point which can be identified by secondary derivative =0. The difference between local minimum is that they have a non zero second derivative number.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok but be careful with respect to what you mean by secondary derivative. You are looking for the secondary partial derivative of the reaction co ordinate with respect to the energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:49, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. ===&lt;br /&gt;
My best estimate of the transition state position &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;&#039;&#039;&#039;= 90.8 pm and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
According to the theory, when the structure is at transition structure, the trajectory point will only oscillate at on point.&lt;br /&gt;
&lt;br /&gt;
[[File:Dist vs time2.png]]&lt;br /&gt;
&lt;br /&gt;
The diagram above is the &#039;internuclear distance vs time&#039; plot for my best estimation of the positions. As shown on the diagram, there is almost no oscillation of the bond distances between B-C and A-B which means&lt;br /&gt;
&lt;br /&gt;
the structure is under a &#039;stable&#039; state and this structure is called transition state structure.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what did you use to approximate this value or get closer to it?  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:53, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 3. Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ. ===&lt;br /&gt;
In my case, positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;91.8&#039;&#039;&#039; pm,  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;90.8 &#039;&#039;&#039;pm and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the new trajectory calculated.&lt;br /&gt;
&lt;br /&gt;
[[File:6_01541238.png]][[File:4_2_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Compare with two diagrams, the MEP doesn&#039;t have the vibrations of the atoms during the process while the trajectory shows oscillation to the products. And other remains the same, both direct to the same product.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, how do the calculation methods differ? The MEP resets the momentum to 0 with each step.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:57, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 4. Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ===&lt;br /&gt;
For the initial positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 74 pm and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 200 pm&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
7_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|unreactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
8_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Don&#039;t have enough energy to overcome the activation barrier, bounce&lt;br /&gt;
back to the more energy preferred state.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
9_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
10_2_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is much higher than the previous ones. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
twice and back to the initial conditions.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
11_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is higher than the previous one. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
three times and complete the reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You could have described the trajectories with slightly more detail.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The table above list some occasions for the different initial energies for the system. The table shows the energy is critically controlled in order to make the reaction complete.&lt;br /&gt;
&lt;br /&gt;
The total energy can&#039;t be too low so that can&#039;t pass though the energy barrier or too high to bounce back even through the transition state point twice.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, what energy prevents the stable formation of the products? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 5. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
With compare with experimental values, the Transition State Theory predictions will be over-estimated. Transition State Theory assumes the transition state structure will not go back to the initial reactants since the transition &lt;br /&gt;
&lt;br /&gt;
structure is formed. An equilibrium will form between the reactants and the transition states. However, in real life there is barrier recrossing cause the transition state structure goes back.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful what you mean by &#039;real life&#039;, do you mean in reference the modelled system or an actual reaction? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Moreover, the Transition State Theory is treated classically Quantum mechanical effect like tunnelling effect is ignored. In real situations, particles with lower kinetic energy might able to cross the high energy barrier caused &lt;br /&gt;
&lt;br /&gt;
by tunnelling effect. Transition State Theory may overestimate the rate because it requires more energy to overcome the barrier.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You are correct that TST will overestimate the rate, but how do th results in the table relate to TST? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 6. By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?  ===&lt;br /&gt;
[[File:12_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
As shown in the diagram above, it is a potential energy surfaces for F + H2 system. The LHS is for HF energy level which is lower than H2 energy level on the RHS. Because the F-H bond is stronger than H-H bond for &lt;br /&gt;
&lt;br /&gt;
F + H2 reaction is endothermic as stronger F-H bond formation required energy. Vice Versa, H + HF reaction is exothermic for strong H-F bond is broke.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| I tihnk you may have misinterpeted the PES here. F + H2 is an exothermic reaction. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:10, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 7. Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
[[File:13_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Diagram above is the &#039;internuclear distance vs time&#039; for my estimated transition state structure.&lt;br /&gt;
&lt;br /&gt;
My best estimated transition state positions are F-H = 180.8 pm and H-H = 74.5 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, you need to make it clear how you calculated this or what you did to get closer to your answer. This answer is correct though, well done for including th einternuclear vs time. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 8. Report the activation energy for both reactions. ===&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;reaction, the activation energy is the energy differences between reactant and transition state structure. &lt;br /&gt;
&lt;br /&gt;
Ea=1.075 kJ/mol&lt;br /&gt;
&lt;br /&gt;
For H + HF reaction,&lt;br /&gt;
&lt;br /&gt;
Ea=126.682 kJ/mol&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Similar to the previous comment, you need to make it clear how you determined the energy of the TS and reactant / product. You could have included an energy vs time plot to show this.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:14, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 9. In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
[[File:14_01541238.png]][[File:15_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:16_01541238.png]][[File:17_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
For the F + H2 reaction. It is an exothermic reaction as the strong F-H bond formed. The potential energy will transfer to kinetic energy in order to complete the reaction. &lt;br /&gt;
&lt;br /&gt;
On diagram 1, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It shows that F-H bond is formed then break apart. Potential energy is transferred to kinetic energy that cause the recrossing &lt;br /&gt;
&lt;br /&gt;
barrier and go back to initial structure as the kinetic energy is too large. &lt;br /&gt;
&lt;br /&gt;
On diagram 2, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The diagram clearly shows 0.526 kJ kinetic energy is transferred which is lower than Activation energy and the reaction can&#039;t&lt;br /&gt;
&lt;br /&gt;
happen. F-H bond not formed.&lt;br /&gt;
&lt;br /&gt;
On diagram 3, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. F-H bond is formed after several formation and breakage. A significant amount of potential energy transfer into kinetic energy &lt;br /&gt;
&lt;br /&gt;
cause the oscillation for the middle H atom during the reaction.&lt;br /&gt;
&lt;br /&gt;
On diagram 4, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.6 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Kinetic energy is 1.707 kJ/mol overcomes the activation barrier and from the F-H bond.&lt;br /&gt;
&lt;br /&gt;
[[File:18_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
On the reverse reaction H + HF, the initial set is H-H = 230 pm and H-F = 100 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -20 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This diagram is one possible reactive trajectory for the reaction to complete. H atom carries 380.526 kJ/mol&lt;br /&gt;
&lt;br /&gt;
to collide with H-F molecule and form new H-H bond.&lt;br /&gt;
&lt;br /&gt;
In conclusion, the kinetic energy can be expressed as temperature. As the potential energy is transferred into kinetic energy, temperature will raise as the result of kinetic energy increases. Monitoring the temperature can help us&lt;br /&gt;
&lt;br /&gt;
to confirm this mechanism processes.&lt;br /&gt;
&lt;br /&gt;
=== Question 10. Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
Translational energy is due to the change in positions and states while vibrational energy is due to the change in structure of molecules. In fact, the translation energy is more effective in promoting reactions for system with early&lt;br /&gt;
&lt;br /&gt;
barrier, whereas vibrational energy is more effective for reactions with late barrier. The position of the transition state is at the top of the activation energy barrier curve on a energy-process diagram. As a result, if the transition state&lt;br /&gt;
&lt;br /&gt;
structure is similar to reactant (early barrier) translational energy is more effective. Vice Versa, if the transition state structure is more similar to the product (late barrier) vibrational energy is more effective. Moreover, symmetric &lt;br /&gt;
&lt;br /&gt;
structure always have higher reaction rate and reactivity than unsymmetric structure.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812777</id>
		<title>MRD:01541238</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812777"/>
		<updated>2020-06-04T19:12:37Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 7. Locate the approximate position of the transition state. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= The Molecular reaction dynamics computational lab report =&lt;br /&gt;
&lt;br /&gt;
=== Question 1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
[[File:1.png]][[File:2.png]]&lt;br /&gt;
&lt;br /&gt;
These two diagrams are the counter plot and skew plot from a three H atoms model. A H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system.&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface diagram (gallery 2). The black reaction trajectory line shows the minimum energy path of the reactants to the products.&lt;br /&gt;
&lt;br /&gt;
When the trajectory line pass through the transition structure it shows a wavy line. And the transition state is defined as the maximum on the black trajectory minimum energy path.&lt;br /&gt;
&lt;br /&gt;
Mathematically the transition state point has the special property that ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 and the energy is higher than any other local minimum points on the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
And the transition state point is a critical point which can be identified by secondary derivative =0. The difference between local minimum is that they have a non zero second derivative number.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok but be careful with respect to what you mean by secondary derivative. You are looking for the secondary partial derivative of the reaction co ordinate with respect to the energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:49, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. ===&lt;br /&gt;
My best estimate of the transition state position &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;&#039;&#039;&#039;= 90.8 pm and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
According to the theory, when the structure is at transition structure, the trajectory point will only oscillate at on point.&lt;br /&gt;
&lt;br /&gt;
[[File:Dist vs time2.png]]&lt;br /&gt;
&lt;br /&gt;
The diagram above is the &#039;internuclear distance vs time&#039; plot for my best estimation of the positions. As shown on the diagram, there is almost no oscillation of the bond distances between B-C and A-B which means&lt;br /&gt;
&lt;br /&gt;
the structure is under a &#039;stable&#039; state and this structure is called transition state structure.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what did you use to approximate this value or get closer to it?  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:53, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 3. Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ. ===&lt;br /&gt;
In my case, positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;91.8&#039;&#039;&#039; pm,  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;90.8 &#039;&#039;&#039;pm and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the new trajectory calculated.&lt;br /&gt;
&lt;br /&gt;
[[File:6_01541238.png]][[File:4_2_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Compare with two diagrams, the MEP doesn&#039;t have the vibrations of the atoms during the process while the trajectory shows oscillation to the products. And other remains the same, both direct to the same product.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, how do the calculation methods differ? The MEP resets the momentum to 0 with each step.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:57, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 4. Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ===&lt;br /&gt;
For the initial positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 74 pm and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 200 pm&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
7_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|unreactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
8_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Don&#039;t have enough energy to overcome the activation barrier, bounce&lt;br /&gt;
back to the more energy preferred state.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
9_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
10_2_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is much higher than the previous ones. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
twice and back to the initial conditions.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
11_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is higher than the previous one. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
three times and complete the reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You could have described the trajectories with slightly more detail.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The table above list some occasions for the different initial energies for the system. The table shows the energy is critically controlled in order to make the reaction complete.&lt;br /&gt;
&lt;br /&gt;
The total energy can&#039;t be too low so that can&#039;t pass though the energy barrier or too high to bounce back even through the transition state point twice.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, what energy prevents the stable formation of the products? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 5. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
With compare with experimental values, the Transition State Theory predictions will be over-estimated. Transition State Theory assumes the transition state structure will not go back to the initial reactants since the transition &lt;br /&gt;
&lt;br /&gt;
structure is formed. An equilibrium will form between the reactants and the transition states. However, in real life there is barrier recrossing cause the transition state structure goes back.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful what you mean by &#039;real life&#039;, do you mean in reference the modelled system or an actual reaction? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Moreover, the Transition State Theory is treated classically Quantum mechanical effect like tunnelling effect is ignored. In real situations, particles with lower kinetic energy might able to cross the high energy barrier caused &lt;br /&gt;
&lt;br /&gt;
by tunnelling effect. Transition State Theory may overestimate the rate because it requires more energy to overcome the barrier.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You are correct that TST will overestimate the rate, but how do th results in the table relate to TST? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 6. By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?  ===&lt;br /&gt;
[[File:12_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
As shown in the diagram above, it is a potential energy surfaces for F + H2 system. The LHS is for HF energy level which is lower than H2 energy level on the RHS. Because the F-H bond is stronger than H-H bond for &lt;br /&gt;
&lt;br /&gt;
F + H2 reaction is endothermic as stronger F-H bond formation required energy. Vice Versa, H + HF reaction is exothermic for strong H-F bond is broke.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| I tihnk you may have misinterpeted the PES here. F + H2 is an exothermic reaction. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:10, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 7. Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
[[File:13_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Diagram above is the &#039;internuclear distance vs time&#039; for my estimated transition state structure.&lt;br /&gt;
&lt;br /&gt;
My best estimated transition state positions are F-H = 180.8 pm and H-H = 74.5 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, you need to make it clear how you calculated this or what you did to get closer to your answer. This answer is correct though, well done for including th einternuclear vs time. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 8. Report the activation energy for both reactions. ===&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;reaction, the activation energy is the energy differences between reactant and transition state structure. &lt;br /&gt;
&lt;br /&gt;
Ea=1.075 kJ/mol&lt;br /&gt;
&lt;br /&gt;
For H + HF reaction,&lt;br /&gt;
&lt;br /&gt;
Ea=126.682 kJ/mol&lt;br /&gt;
&lt;br /&gt;
=== Question 9. In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
[[File:14_01541238.png]][[File:15_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:16_01541238.png]][[File:17_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
For the F + H2 reaction. It is an exothermic reaction as the strong F-H bond formed. The potential energy will transfer to kinetic energy in order to complete the reaction. &lt;br /&gt;
&lt;br /&gt;
On diagram 1, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It shows that F-H bond is formed then break apart. Potential energy is transferred to kinetic energy that cause the recrossing &lt;br /&gt;
&lt;br /&gt;
barrier and go back to initial structure as the kinetic energy is too large. &lt;br /&gt;
&lt;br /&gt;
On diagram 2, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The diagram clearly shows 0.526 kJ kinetic energy is transferred which is lower than Activation energy and the reaction can&#039;t&lt;br /&gt;
&lt;br /&gt;
happen. F-H bond not formed.&lt;br /&gt;
&lt;br /&gt;
On diagram 3, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. F-H bond is formed after several formation and breakage. A significant amount of potential energy transfer into kinetic energy &lt;br /&gt;
&lt;br /&gt;
cause the oscillation for the middle H atom during the reaction.&lt;br /&gt;
&lt;br /&gt;
On diagram 4, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.6 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Kinetic energy is 1.707 kJ/mol overcomes the activation barrier and from the F-H bond.&lt;br /&gt;
&lt;br /&gt;
[[File:18_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
On the reverse reaction H + HF, the initial set is H-H = 230 pm and H-F = 100 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -20 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This diagram is one possible reactive trajectory for the reaction to complete. H atom carries 380.526 kJ/mol&lt;br /&gt;
&lt;br /&gt;
to collide with H-F molecule and form new H-H bond.&lt;br /&gt;
&lt;br /&gt;
In conclusion, the kinetic energy can be expressed as temperature. As the potential energy is transferred into kinetic energy, temperature will raise as the result of kinetic energy increases. Monitoring the temperature can help us&lt;br /&gt;
&lt;br /&gt;
to confirm this mechanism processes.&lt;br /&gt;
&lt;br /&gt;
=== Question 10. Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
Translational energy is due to the change in positions and states while vibrational energy is due to the change in structure of molecules. In fact, the translation energy is more effective in promoting reactions for system with early&lt;br /&gt;
&lt;br /&gt;
barrier, whereas vibrational energy is more effective for reactions with late barrier. The position of the transition state is at the top of the activation energy barrier curve on a energy-process diagram. As a result, if the transition state&lt;br /&gt;
&lt;br /&gt;
structure is similar to reactant (early barrier) translational energy is more effective. Vice Versa, if the transition state structure is more similar to the product (late barrier) vibrational energy is more effective. Moreover, symmetric &lt;br /&gt;
&lt;br /&gt;
structure always have higher reaction rate and reactivity than unsymmetric structure.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812776</id>
		<title>MRD:01541238</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812776"/>
		<updated>2020-06-04T19:10:45Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 6. By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= The Molecular reaction dynamics computational lab report =&lt;br /&gt;
&lt;br /&gt;
=== Question 1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
[[File:1.png]][[File:2.png]]&lt;br /&gt;
&lt;br /&gt;
These two diagrams are the counter plot and skew plot from a three H atoms model. A H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system.&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface diagram (gallery 2). The black reaction trajectory line shows the minimum energy path of the reactants to the products.&lt;br /&gt;
&lt;br /&gt;
When the trajectory line pass through the transition structure it shows a wavy line. And the transition state is defined as the maximum on the black trajectory minimum energy path.&lt;br /&gt;
&lt;br /&gt;
Mathematically the transition state point has the special property that ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 and the energy is higher than any other local minimum points on the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
And the transition state point is a critical point which can be identified by secondary derivative =0. The difference between local minimum is that they have a non zero second derivative number.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok but be careful with respect to what you mean by secondary derivative. You are looking for the secondary partial derivative of the reaction co ordinate with respect to the energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:49, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. ===&lt;br /&gt;
My best estimate of the transition state position &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;&#039;&#039;&#039;= 90.8 pm and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
According to the theory, when the structure is at transition structure, the trajectory point will only oscillate at on point.&lt;br /&gt;
&lt;br /&gt;
[[File:Dist vs time2.png]]&lt;br /&gt;
&lt;br /&gt;
The diagram above is the &#039;internuclear distance vs time&#039; plot for my best estimation of the positions. As shown on the diagram, there is almost no oscillation of the bond distances between B-C and A-B which means&lt;br /&gt;
&lt;br /&gt;
the structure is under a &#039;stable&#039; state and this structure is called transition state structure.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what did you use to approximate this value or get closer to it?  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:53, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 3. Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ. ===&lt;br /&gt;
In my case, positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;91.8&#039;&#039;&#039; pm,  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;90.8 &#039;&#039;&#039;pm and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the new trajectory calculated.&lt;br /&gt;
&lt;br /&gt;
[[File:6_01541238.png]][[File:4_2_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Compare with two diagrams, the MEP doesn&#039;t have the vibrations of the atoms during the process while the trajectory shows oscillation to the products. And other remains the same, both direct to the same product.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, how do the calculation methods differ? The MEP resets the momentum to 0 with each step.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:57, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 4. Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ===&lt;br /&gt;
For the initial positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 74 pm and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 200 pm&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
7_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|unreactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
8_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Don&#039;t have enough energy to overcome the activation barrier, bounce&lt;br /&gt;
back to the more energy preferred state.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
9_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
10_2_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is much higher than the previous ones. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
twice and back to the initial conditions.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
11_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is higher than the previous one. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
three times and complete the reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You could have described the trajectories with slightly more detail.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The table above list some occasions for the different initial energies for the system. The table shows the energy is critically controlled in order to make the reaction complete.&lt;br /&gt;
&lt;br /&gt;
The total energy can&#039;t be too low so that can&#039;t pass though the energy barrier or too high to bounce back even through the transition state point twice.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, what energy prevents the stable formation of the products? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 5. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
With compare with experimental values, the Transition State Theory predictions will be over-estimated. Transition State Theory assumes the transition state structure will not go back to the initial reactants since the transition &lt;br /&gt;
&lt;br /&gt;
structure is formed. An equilibrium will form between the reactants and the transition states. However, in real life there is barrier recrossing cause the transition state structure goes back.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful what you mean by &#039;real life&#039;, do you mean in reference the modelled system or an actual reaction? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Moreover, the Transition State Theory is treated classically Quantum mechanical effect like tunnelling effect is ignored. In real situations, particles with lower kinetic energy might able to cross the high energy barrier caused &lt;br /&gt;
&lt;br /&gt;
by tunnelling effect. Transition State Theory may overestimate the rate because it requires more energy to overcome the barrier.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You are correct that TST will overestimate the rate, but how do th results in the table relate to TST? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 6. By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?  ===&lt;br /&gt;
[[File:12_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
As shown in the diagram above, it is a potential energy surfaces for F + H2 system. The LHS is for HF energy level which is lower than H2 energy level on the RHS. Because the F-H bond is stronger than H-H bond for &lt;br /&gt;
&lt;br /&gt;
F + H2 reaction is endothermic as stronger F-H bond formation required energy. Vice Versa, H + HF reaction is exothermic for strong H-F bond is broke.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| I tihnk you may have misinterpeted the PES here. F + H2 is an exothermic reaction. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:10, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 7. Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
[[File:13_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Diagram above is the &#039;internuclear distance vs time&#039; for my estimated transition state structure.&lt;br /&gt;
&lt;br /&gt;
My best estimated transition state positions are F-H = 180.8 pm and H-H = 74.5 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Question 8. Report the activation energy for both reactions. ===&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;reaction, the activation energy is the energy differences between reactant and transition state structure. &lt;br /&gt;
&lt;br /&gt;
Ea=1.075 kJ/mol&lt;br /&gt;
&lt;br /&gt;
For H + HF reaction,&lt;br /&gt;
&lt;br /&gt;
Ea=126.682 kJ/mol&lt;br /&gt;
&lt;br /&gt;
=== Question 9. In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
[[File:14_01541238.png]][[File:15_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:16_01541238.png]][[File:17_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
For the F + H2 reaction. It is an exothermic reaction as the strong F-H bond formed. The potential energy will transfer to kinetic energy in order to complete the reaction. &lt;br /&gt;
&lt;br /&gt;
On diagram 1, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It shows that F-H bond is formed then break apart. Potential energy is transferred to kinetic energy that cause the recrossing &lt;br /&gt;
&lt;br /&gt;
barrier and go back to initial structure as the kinetic energy is too large. &lt;br /&gt;
&lt;br /&gt;
On diagram 2, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The diagram clearly shows 0.526 kJ kinetic energy is transferred which is lower than Activation energy and the reaction can&#039;t&lt;br /&gt;
&lt;br /&gt;
happen. F-H bond not formed.&lt;br /&gt;
&lt;br /&gt;
On diagram 3, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. F-H bond is formed after several formation and breakage. A significant amount of potential energy transfer into kinetic energy &lt;br /&gt;
&lt;br /&gt;
cause the oscillation for the middle H atom during the reaction.&lt;br /&gt;
&lt;br /&gt;
On diagram 4, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.6 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Kinetic energy is 1.707 kJ/mol overcomes the activation barrier and from the F-H bond.&lt;br /&gt;
&lt;br /&gt;
[[File:18_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
On the reverse reaction H + HF, the initial set is H-H = 230 pm and H-F = 100 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -20 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This diagram is one possible reactive trajectory for the reaction to complete. H atom carries 380.526 kJ/mol&lt;br /&gt;
&lt;br /&gt;
to collide with H-F molecule and form new H-H bond.&lt;br /&gt;
&lt;br /&gt;
In conclusion, the kinetic energy can be expressed as temperature. As the potential energy is transferred into kinetic energy, temperature will raise as the result of kinetic energy increases. Monitoring the temperature can help us&lt;br /&gt;
&lt;br /&gt;
to confirm this mechanism processes.&lt;br /&gt;
&lt;br /&gt;
=== Question 10. Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
Translational energy is due to the change in positions and states while vibrational energy is due to the change in structure of molecules. In fact, the translation energy is more effective in promoting reactions for system with early&lt;br /&gt;
&lt;br /&gt;
barrier, whereas vibrational energy is more effective for reactions with late barrier. The position of the transition state is at the top of the activation energy barrier curve on a energy-process diagram. As a result, if the transition state&lt;br /&gt;
&lt;br /&gt;
structure is similar to reactant (early barrier) translational energy is more effective. Vice Versa, if the transition state structure is more similar to the product (late barrier) vibrational energy is more effective. Moreover, symmetric &lt;br /&gt;
&lt;br /&gt;
structure always have higher reaction rate and reactivity than unsymmetric structure.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812775</id>
		<title>MRD:01541238</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812775"/>
		<updated>2020-06-04T19:04:42Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 5. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= The Molecular reaction dynamics computational lab report =&lt;br /&gt;
&lt;br /&gt;
=== Question 1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
[[File:1.png]][[File:2.png]]&lt;br /&gt;
&lt;br /&gt;
These two diagrams are the counter plot and skew plot from a three H atoms model. A H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system.&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface diagram (gallery 2). The black reaction trajectory line shows the minimum energy path of the reactants to the products.&lt;br /&gt;
&lt;br /&gt;
When the trajectory line pass through the transition structure it shows a wavy line. And the transition state is defined as the maximum on the black trajectory minimum energy path.&lt;br /&gt;
&lt;br /&gt;
Mathematically the transition state point has the special property that ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 and the energy is higher than any other local minimum points on the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
And the transition state point is a critical point which can be identified by secondary derivative =0. The difference between local minimum is that they have a non zero second derivative number.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok but be careful with respect to what you mean by secondary derivative. You are looking for the secondary partial derivative of the reaction co ordinate with respect to the energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:49, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. ===&lt;br /&gt;
My best estimate of the transition state position &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;&#039;&#039;&#039;= 90.8 pm and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
According to the theory, when the structure is at transition structure, the trajectory point will only oscillate at on point.&lt;br /&gt;
&lt;br /&gt;
[[File:Dist vs time2.png]]&lt;br /&gt;
&lt;br /&gt;
The diagram above is the &#039;internuclear distance vs time&#039; plot for my best estimation of the positions. As shown on the diagram, there is almost no oscillation of the bond distances between B-C and A-B which means&lt;br /&gt;
&lt;br /&gt;
the structure is under a &#039;stable&#039; state and this structure is called transition state structure.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what did you use to approximate this value or get closer to it?  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:53, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 3. Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ. ===&lt;br /&gt;
In my case, positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;91.8&#039;&#039;&#039; pm,  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;90.8 &#039;&#039;&#039;pm and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the new trajectory calculated.&lt;br /&gt;
&lt;br /&gt;
[[File:6_01541238.png]][[File:4_2_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Compare with two diagrams, the MEP doesn&#039;t have the vibrations of the atoms during the process while the trajectory shows oscillation to the products. And other remains the same, both direct to the same product.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, how do the calculation methods differ? The MEP resets the momentum to 0 with each step.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:57, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 4. Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ===&lt;br /&gt;
For the initial positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 74 pm and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 200 pm&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
7_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|unreactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
8_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Don&#039;t have enough energy to overcome the activation barrier, bounce&lt;br /&gt;
back to the more energy preferred state.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
9_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
10_2_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is much higher than the previous ones. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
twice and back to the initial conditions.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
11_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is higher than the previous one. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
three times and complete the reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You could have described the trajectories with slightly more detail.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The table above list some occasions for the different initial energies for the system. The table shows the energy is critically controlled in order to make the reaction complete.&lt;br /&gt;
&lt;br /&gt;
The total energy can&#039;t be too low so that can&#039;t pass though the energy barrier or too high to bounce back even through the transition state point twice.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, what energy prevents the stable formation of the products? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 5. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
With compare with experimental values, the Transition State Theory predictions will be over-estimated. Transition State Theory assumes the transition state structure will not go back to the initial reactants since the transition &lt;br /&gt;
&lt;br /&gt;
structure is formed. An equilibrium will form between the reactants and the transition states. However, in real life there is barrier recrossing cause the transition state structure goes back.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful what you mean by &#039;real life&#039;, do you mean in reference the modelled system or an actual reaction? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Moreover, the Transition State Theory is treated classically Quantum mechanical effect like tunnelling effect is ignored. In real situations, particles with lower kinetic energy might able to cross the high energy barrier caused &lt;br /&gt;
&lt;br /&gt;
by tunnelling effect. Transition State Theory may overestimate the rate because it requires more energy to overcome the barrier.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You are correct that TST will overestimate the rate, but how do th results in the table relate to TST? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 6. By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?  ===&lt;br /&gt;
[[File:12_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
As shown in the diagram above, it is a potential energy surfaces for F + H2 system. The LHS is for HF energy level which is lower than H2 energy level on the RHS. Because the F-H bond is stronger than H-H bond for &lt;br /&gt;
&lt;br /&gt;
F + H2 reaction is endothermic as stronger F-H bond formation required energy. Vice Versa, H + HF reaction is exothermic for strong H-F bond is broke.&lt;br /&gt;
&lt;br /&gt;
=== Question 7. Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
[[File:13_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Diagram above is the &#039;internuclear distance vs time&#039; for my estimated transition state structure.&lt;br /&gt;
&lt;br /&gt;
My best estimated transition state positions are F-H = 180.8 pm and H-H = 74.5 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Question 8. Report the activation energy for both reactions. ===&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;reaction, the activation energy is the energy differences between reactant and transition state structure. &lt;br /&gt;
&lt;br /&gt;
Ea=1.075 kJ/mol&lt;br /&gt;
&lt;br /&gt;
For H + HF reaction,&lt;br /&gt;
&lt;br /&gt;
Ea=126.682 kJ/mol&lt;br /&gt;
&lt;br /&gt;
=== Question 9. In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
[[File:14_01541238.png]][[File:15_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:16_01541238.png]][[File:17_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
For the F + H2 reaction. It is an exothermic reaction as the strong F-H bond formed. The potential energy will transfer to kinetic energy in order to complete the reaction. &lt;br /&gt;
&lt;br /&gt;
On diagram 1, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It shows that F-H bond is formed then break apart. Potential energy is transferred to kinetic energy that cause the recrossing &lt;br /&gt;
&lt;br /&gt;
barrier and go back to initial structure as the kinetic energy is too large. &lt;br /&gt;
&lt;br /&gt;
On diagram 2, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The diagram clearly shows 0.526 kJ kinetic energy is transferred which is lower than Activation energy and the reaction can&#039;t&lt;br /&gt;
&lt;br /&gt;
happen. F-H bond not formed.&lt;br /&gt;
&lt;br /&gt;
On diagram 3, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. F-H bond is formed after several formation and breakage. A significant amount of potential energy transfer into kinetic energy &lt;br /&gt;
&lt;br /&gt;
cause the oscillation for the middle H atom during the reaction.&lt;br /&gt;
&lt;br /&gt;
On diagram 4, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.6 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Kinetic energy is 1.707 kJ/mol overcomes the activation barrier and from the F-H bond.&lt;br /&gt;
&lt;br /&gt;
[[File:18_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
On the reverse reaction H + HF, the initial set is H-H = 230 pm and H-F = 100 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -20 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This diagram is one possible reactive trajectory for the reaction to complete. H atom carries 380.526 kJ/mol&lt;br /&gt;
&lt;br /&gt;
to collide with H-F molecule and form new H-H bond.&lt;br /&gt;
&lt;br /&gt;
In conclusion, the kinetic energy can be expressed as temperature. As the potential energy is transferred into kinetic energy, temperature will raise as the result of kinetic energy increases. Monitoring the temperature can help us&lt;br /&gt;
&lt;br /&gt;
to confirm this mechanism processes.&lt;br /&gt;
&lt;br /&gt;
=== Question 10. Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
Translational energy is due to the change in positions and states while vibrational energy is due to the change in structure of molecules. In fact, the translation energy is more effective in promoting reactions for system with early&lt;br /&gt;
&lt;br /&gt;
barrier, whereas vibrational energy is more effective for reactions with late barrier. The position of the transition state is at the top of the activation energy barrier curve on a energy-process diagram. As a result, if the transition state&lt;br /&gt;
&lt;br /&gt;
structure is similar to reactant (early barrier) translational energy is more effective. Vice Versa, if the transition state structure is more similar to the product (late barrier) vibrational energy is more effective. Moreover, symmetric &lt;br /&gt;
&lt;br /&gt;
structure always have higher reaction rate and reactivity than unsymmetric structure.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812774</id>
		<title>MRD:01541238</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812774"/>
		<updated>2020-06-04T19:02:24Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 4. Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the tab...&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= The Molecular reaction dynamics computational lab report =&lt;br /&gt;
&lt;br /&gt;
=== Question 1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
[[File:1.png]][[File:2.png]]&lt;br /&gt;
&lt;br /&gt;
These two diagrams are the counter plot and skew plot from a three H atoms model. A H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system.&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface diagram (gallery 2). The black reaction trajectory line shows the minimum energy path of the reactants to the products.&lt;br /&gt;
&lt;br /&gt;
When the trajectory line pass through the transition structure it shows a wavy line. And the transition state is defined as the maximum on the black trajectory minimum energy path.&lt;br /&gt;
&lt;br /&gt;
Mathematically the transition state point has the special property that ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 and the energy is higher than any other local minimum points on the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
And the transition state point is a critical point which can be identified by secondary derivative =0. The difference between local minimum is that they have a non zero second derivative number.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok but be careful with respect to what you mean by secondary derivative. You are looking for the secondary partial derivative of the reaction co ordinate with respect to the energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:49, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. ===&lt;br /&gt;
My best estimate of the transition state position &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;&#039;&#039;&#039;= 90.8 pm and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
According to the theory, when the structure is at transition structure, the trajectory point will only oscillate at on point.&lt;br /&gt;
&lt;br /&gt;
[[File:Dist vs time2.png]]&lt;br /&gt;
&lt;br /&gt;
The diagram above is the &#039;internuclear distance vs time&#039; plot for my best estimation of the positions. As shown on the diagram, there is almost no oscillation of the bond distances between B-C and A-B which means&lt;br /&gt;
&lt;br /&gt;
the structure is under a &#039;stable&#039; state and this structure is called transition state structure.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what did you use to approximate this value or get closer to it?  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:53, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 3. Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ. ===&lt;br /&gt;
In my case, positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;91.8&#039;&#039;&#039; pm,  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;90.8 &#039;&#039;&#039;pm and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the new trajectory calculated.&lt;br /&gt;
&lt;br /&gt;
[[File:6_01541238.png]][[File:4_2_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Compare with two diagrams, the MEP doesn&#039;t have the vibrations of the atoms during the process while the trajectory shows oscillation to the products. And other remains the same, both direct to the same product.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, how do the calculation methods differ? The MEP resets the momentum to 0 with each step.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:57, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 4. Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ===&lt;br /&gt;
For the initial positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 74 pm and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 200 pm&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
7_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|unreactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
8_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Don&#039;t have enough energy to overcome the activation barrier, bounce&lt;br /&gt;
back to the more energy preferred state.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
9_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
10_2_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is much higher than the previous ones. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
twice and back to the initial conditions.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
11_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is higher than the previous one. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
three times and complete the reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| You could have described the trajectories with slightly more detail.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The table above list some occasions for the different initial energies for the system. The table shows the energy is critically controlled in order to make the reaction complete.&lt;br /&gt;
&lt;br /&gt;
The total energy can&#039;t be too low so that can&#039;t pass though the energy barrier or too high to bounce back even through the transition state point twice.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, what energy prevents the stable formation of the products? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 20:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 5. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
With compare with experimental values, the Transition State Theory predictions will be over-estimated. Transition State Theory assumes the transition state structure will not go back to the initial reactants since the transition &lt;br /&gt;
&lt;br /&gt;
structure is formed. An equilibrium will form between the reactants and the transition states. However, in real life there is barrier recrossing cause the transition state structure goes back.&lt;br /&gt;
&lt;br /&gt;
Moreover, the Transition State Theory is treated classically Quantum mechanical effect like tunnelling effect is ignored. In real situations, particles with lower kinetic energy might able to cross the high energy barrier caused &lt;br /&gt;
&lt;br /&gt;
by tunnelling effect. Transition State Theory may overestimate the rate because it requires more energy to overcome the barrier.&lt;br /&gt;
&lt;br /&gt;
=== Question 6. By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?  ===&lt;br /&gt;
[[File:12_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
As shown in the diagram above, it is a potential energy surfaces for F + H2 system. The LHS is for HF energy level which is lower than H2 energy level on the RHS. Because the F-H bond is stronger than H-H bond for &lt;br /&gt;
&lt;br /&gt;
F + H2 reaction is endothermic as stronger F-H bond formation required energy. Vice Versa, H + HF reaction is exothermic for strong H-F bond is broke.&lt;br /&gt;
&lt;br /&gt;
=== Question 7. Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
[[File:13_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Diagram above is the &#039;internuclear distance vs time&#039; for my estimated transition state structure.&lt;br /&gt;
&lt;br /&gt;
My best estimated transition state positions are F-H = 180.8 pm and H-H = 74.5 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Question 8. Report the activation energy for both reactions. ===&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;reaction, the activation energy is the energy differences between reactant and transition state structure. &lt;br /&gt;
&lt;br /&gt;
Ea=1.075 kJ/mol&lt;br /&gt;
&lt;br /&gt;
For H + HF reaction,&lt;br /&gt;
&lt;br /&gt;
Ea=126.682 kJ/mol&lt;br /&gt;
&lt;br /&gt;
=== Question 9. In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
[[File:14_01541238.png]][[File:15_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:16_01541238.png]][[File:17_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
For the F + H2 reaction. It is an exothermic reaction as the strong F-H bond formed. The potential energy will transfer to kinetic energy in order to complete the reaction. &lt;br /&gt;
&lt;br /&gt;
On diagram 1, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It shows that F-H bond is formed then break apart. Potential energy is transferred to kinetic energy that cause the recrossing &lt;br /&gt;
&lt;br /&gt;
barrier and go back to initial structure as the kinetic energy is too large. &lt;br /&gt;
&lt;br /&gt;
On diagram 2, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The diagram clearly shows 0.526 kJ kinetic energy is transferred which is lower than Activation energy and the reaction can&#039;t&lt;br /&gt;
&lt;br /&gt;
happen. F-H bond not formed.&lt;br /&gt;
&lt;br /&gt;
On diagram 3, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. F-H bond is formed after several formation and breakage. A significant amount of potential energy transfer into kinetic energy &lt;br /&gt;
&lt;br /&gt;
cause the oscillation for the middle H atom during the reaction.&lt;br /&gt;
&lt;br /&gt;
On diagram 4, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.6 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Kinetic energy is 1.707 kJ/mol overcomes the activation barrier and from the F-H bond.&lt;br /&gt;
&lt;br /&gt;
[[File:18_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
On the reverse reaction H + HF, the initial set is H-H = 230 pm and H-F = 100 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -20 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This diagram is one possible reactive trajectory for the reaction to complete. H atom carries 380.526 kJ/mol&lt;br /&gt;
&lt;br /&gt;
to collide with H-F molecule and form new H-H bond.&lt;br /&gt;
&lt;br /&gt;
In conclusion, the kinetic energy can be expressed as temperature. As the potential energy is transferred into kinetic energy, temperature will raise as the result of kinetic energy increases. Monitoring the temperature can help us&lt;br /&gt;
&lt;br /&gt;
to confirm this mechanism processes.&lt;br /&gt;
&lt;br /&gt;
=== Question 10. Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
Translational energy is due to the change in positions and states while vibrational energy is due to the change in structure of molecules. In fact, the translation energy is more effective in promoting reactions for system with early&lt;br /&gt;
&lt;br /&gt;
barrier, whereas vibrational energy is more effective for reactions with late barrier. The position of the transition state is at the top of the activation energy barrier curve on a energy-process diagram. As a result, if the transition state&lt;br /&gt;
&lt;br /&gt;
structure is similar to reactant (early barrier) translational energy is more effective. Vice Versa, if the transition state structure is more similar to the product (late barrier) vibrational energy is more effective. Moreover, symmetric &lt;br /&gt;
&lt;br /&gt;
structure always have higher reaction rate and reactivity than unsymmetric structure.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812773</id>
		<title>MRD:01541238</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812773"/>
		<updated>2020-06-04T18:57:12Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 3. Comment on how the mep and the trajectory you just calculated differ. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= The Molecular reaction dynamics computational lab report =&lt;br /&gt;
&lt;br /&gt;
=== Question 1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
[[File:1.png]][[File:2.png]]&lt;br /&gt;
&lt;br /&gt;
These two diagrams are the counter plot and skew plot from a three H atoms model. A H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system.&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface diagram (gallery 2). The black reaction trajectory line shows the minimum energy path of the reactants to the products.&lt;br /&gt;
&lt;br /&gt;
When the trajectory line pass through the transition structure it shows a wavy line. And the transition state is defined as the maximum on the black trajectory minimum energy path.&lt;br /&gt;
&lt;br /&gt;
Mathematically the transition state point has the special property that ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 and the energy is higher than any other local minimum points on the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
And the transition state point is a critical point which can be identified by secondary derivative =0. The difference between local minimum is that they have a non zero second derivative number.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok but be careful with respect to what you mean by secondary derivative. You are looking for the secondary partial derivative of the reaction co ordinate with respect to the energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:49, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. ===&lt;br /&gt;
My best estimate of the transition state position &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;&#039;&#039;&#039;= 90.8 pm and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
According to the theory, when the structure is at transition structure, the trajectory point will only oscillate at on point.&lt;br /&gt;
&lt;br /&gt;
[[File:Dist vs time2.png]]&lt;br /&gt;
&lt;br /&gt;
The diagram above is the &#039;internuclear distance vs time&#039; plot for my best estimation of the positions. As shown on the diagram, there is almost no oscillation of the bond distances between B-C and A-B which means&lt;br /&gt;
&lt;br /&gt;
the structure is under a &#039;stable&#039; state and this structure is called transition state structure.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what did you use to approximate this value or get closer to it?  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:53, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 3. Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ. ===&lt;br /&gt;
In my case, positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;91.8&#039;&#039;&#039; pm,  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;90.8 &#039;&#039;&#039;pm and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the new trajectory calculated.&lt;br /&gt;
&lt;br /&gt;
[[File:6_01541238.png]][[File:4_2_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Compare with two diagrams, the MEP doesn&#039;t have the vibrations of the atoms during the process while the trajectory shows oscillation to the products. And other remains the same, both direct to the same product.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, how do the calculation methods differ? The MEP resets the momentum to 0 with each step.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:57, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 4. Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ===&lt;br /&gt;
For the initial positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 74 pm and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 200 pm&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
7_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|unreactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
8_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Don&#039;t have enough energy to overcome the activation barrier, bounce&lt;br /&gt;
back to the more energy preferred state.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
9_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
10_2_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is much higher than the previous ones. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
twice and back to the initial conditions.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
11_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is higher than the previous one. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
three times and complete the reaction.&lt;br /&gt;
|}&lt;br /&gt;
The table above list some occasions for the different initial energies for the system. The table shows the energy is critically controlled in order to make the reaction complete.&lt;br /&gt;
&lt;br /&gt;
The total energy can&#039;t be too low so that can&#039;t pass though the energy barrier or too high to bounce back even through the transition state point twice. &lt;br /&gt;
&lt;br /&gt;
=== Question 5. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
With compare with experimental values, the Transition State Theory predictions will be over-estimated. Transition State Theory assumes the transition state structure will not go back to the initial reactants since the transition &lt;br /&gt;
&lt;br /&gt;
structure is formed. An equilibrium will form between the reactants and the transition states. However, in real life there is barrier recrossing cause the transition state structure goes back.&lt;br /&gt;
&lt;br /&gt;
Moreover, the Transition State Theory is treated classically Quantum mechanical effect like tunnelling effect is ignored. In real situations, particles with lower kinetic energy might able to cross the high energy barrier caused &lt;br /&gt;
&lt;br /&gt;
by tunnelling effect. Transition State Theory may overestimate the rate because it requires more energy to overcome the barrier.&lt;br /&gt;
&lt;br /&gt;
=== Question 6. By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?  ===&lt;br /&gt;
[[File:12_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
As shown in the diagram above, it is a potential energy surfaces for F + H2 system. The LHS is for HF energy level which is lower than H2 energy level on the RHS. Because the F-H bond is stronger than H-H bond for &lt;br /&gt;
&lt;br /&gt;
F + H2 reaction is endothermic as stronger F-H bond formation required energy. Vice Versa, H + HF reaction is exothermic for strong H-F bond is broke.&lt;br /&gt;
&lt;br /&gt;
=== Question 7. Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
[[File:13_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Diagram above is the &#039;internuclear distance vs time&#039; for my estimated transition state structure.&lt;br /&gt;
&lt;br /&gt;
My best estimated transition state positions are F-H = 180.8 pm and H-H = 74.5 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Question 8. Report the activation energy for both reactions. ===&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;reaction, the activation energy is the energy differences between reactant and transition state structure. &lt;br /&gt;
&lt;br /&gt;
Ea=1.075 kJ/mol&lt;br /&gt;
&lt;br /&gt;
For H + HF reaction,&lt;br /&gt;
&lt;br /&gt;
Ea=126.682 kJ/mol&lt;br /&gt;
&lt;br /&gt;
=== Question 9. In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
[[File:14_01541238.png]][[File:15_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:16_01541238.png]][[File:17_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
For the F + H2 reaction. It is an exothermic reaction as the strong F-H bond formed. The potential energy will transfer to kinetic energy in order to complete the reaction. &lt;br /&gt;
&lt;br /&gt;
On diagram 1, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It shows that F-H bond is formed then break apart. Potential energy is transferred to kinetic energy that cause the recrossing &lt;br /&gt;
&lt;br /&gt;
barrier and go back to initial structure as the kinetic energy is too large. &lt;br /&gt;
&lt;br /&gt;
On diagram 2, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The diagram clearly shows 0.526 kJ kinetic energy is transferred which is lower than Activation energy and the reaction can&#039;t&lt;br /&gt;
&lt;br /&gt;
happen. F-H bond not formed.&lt;br /&gt;
&lt;br /&gt;
On diagram 3, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. F-H bond is formed after several formation and breakage. A significant amount of potential energy transfer into kinetic energy &lt;br /&gt;
&lt;br /&gt;
cause the oscillation for the middle H atom during the reaction.&lt;br /&gt;
&lt;br /&gt;
On diagram 4, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.6 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Kinetic energy is 1.707 kJ/mol overcomes the activation barrier and from the F-H bond.&lt;br /&gt;
&lt;br /&gt;
[[File:18_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
On the reverse reaction H + HF, the initial set is H-H = 230 pm and H-F = 100 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -20 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This diagram is one possible reactive trajectory for the reaction to complete. H atom carries 380.526 kJ/mol&lt;br /&gt;
&lt;br /&gt;
to collide with H-F molecule and form new H-H bond.&lt;br /&gt;
&lt;br /&gt;
In conclusion, the kinetic energy can be expressed as temperature. As the potential energy is transferred into kinetic energy, temperature will raise as the result of kinetic energy increases. Monitoring the temperature can help us&lt;br /&gt;
&lt;br /&gt;
to confirm this mechanism processes.&lt;br /&gt;
&lt;br /&gt;
=== Question 10. Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
Translational energy is due to the change in positions and states while vibrational energy is due to the change in structure of molecules. In fact, the translation energy is more effective in promoting reactions for system with early&lt;br /&gt;
&lt;br /&gt;
barrier, whereas vibrational energy is more effective for reactions with late barrier. The position of the transition state is at the top of the activation energy barrier curve on a energy-process diagram. As a result, if the transition state&lt;br /&gt;
&lt;br /&gt;
structure is similar to reactant (early barrier) translational energy is more effective. Vice Versa, if the transition state structure is more similar to the product (late barrier) vibrational energy is more effective. Moreover, symmetric &lt;br /&gt;
&lt;br /&gt;
structure always have higher reaction rate and reactivity than unsymmetric structure.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812772</id>
		<title>MRD:01541238</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812772"/>
		<updated>2020-06-04T18:54:28Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 2. Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= The Molecular reaction dynamics computational lab report =&lt;br /&gt;
&lt;br /&gt;
=== Question 1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
[[File:1.png]][[File:2.png]]&lt;br /&gt;
&lt;br /&gt;
These two diagrams are the counter plot and skew plot from a three H atoms model. A H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system.&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface diagram (gallery 2). The black reaction trajectory line shows the minimum energy path of the reactants to the products.&lt;br /&gt;
&lt;br /&gt;
When the trajectory line pass through the transition structure it shows a wavy line. And the transition state is defined as the maximum on the black trajectory minimum energy path.&lt;br /&gt;
&lt;br /&gt;
Mathematically the transition state point has the special property that ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 and the energy is higher than any other local minimum points on the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
And the transition state point is a critical point which can be identified by secondary derivative =0. The difference between local minimum is that they have a non zero second derivative number.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok but be careful with respect to what you mean by secondary derivative. You are looking for the secondary partial derivative of the reaction co ordinate with respect to the energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:49, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. ===&lt;br /&gt;
My best estimate of the transition state position &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;&#039;&#039;&#039;= 90.8 pm and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
According to the theory, when the structure is at transition structure, the trajectory point will only oscillate at on point.&lt;br /&gt;
&lt;br /&gt;
[[File:Dist vs time2.png]]&lt;br /&gt;
&lt;br /&gt;
The diagram above is the &#039;internuclear distance vs time&#039; plot for my best estimation of the positions. As shown on the diagram, there is almost no oscillation of the bond distances between B-C and A-B which means&lt;br /&gt;
&lt;br /&gt;
the structure is under a &#039;stable&#039; state and this structure is called transition state structure.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what did you use to approximate this value or get closer to it?  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:53, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 3. Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ. ===&lt;br /&gt;
In my case, positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;91.8&#039;&#039;&#039; pm,  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;90.8 &#039;&#039;&#039;pm and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the new trajectory calculated.&lt;br /&gt;
&lt;br /&gt;
[[File:6_01541238.png]][[File:4_2_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Compare with two diagrams, the MEP doesn&#039;t have the vibrations of the atoms during the process while the trajectory shows oscillation to the products. And other remains the same, both direct to the same product.&lt;br /&gt;
&lt;br /&gt;
=== Question 4. Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ===&lt;br /&gt;
For the initial positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 74 pm and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 200 pm&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
7_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|unreactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
8_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Don&#039;t have enough energy to overcome the activation barrier, bounce&lt;br /&gt;
back to the more energy preferred state.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
9_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
10_2_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is much higher than the previous ones. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
twice and back to the initial conditions.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
11_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is higher than the previous one. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
three times and complete the reaction.&lt;br /&gt;
|}&lt;br /&gt;
The table above list some occasions for the different initial energies for the system. The table shows the energy is critically controlled in order to make the reaction complete.&lt;br /&gt;
&lt;br /&gt;
The total energy can&#039;t be too low so that can&#039;t pass though the energy barrier or too high to bounce back even through the transition state point twice. &lt;br /&gt;
&lt;br /&gt;
=== Question 5. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
With compare with experimental values, the Transition State Theory predictions will be over-estimated. Transition State Theory assumes the transition state structure will not go back to the initial reactants since the transition &lt;br /&gt;
&lt;br /&gt;
structure is formed. An equilibrium will form between the reactants and the transition states. However, in real life there is barrier recrossing cause the transition state structure goes back.&lt;br /&gt;
&lt;br /&gt;
Moreover, the Transition State Theory is treated classically Quantum mechanical effect like tunnelling effect is ignored. In real situations, particles with lower kinetic energy might able to cross the high energy barrier caused &lt;br /&gt;
&lt;br /&gt;
by tunnelling effect. Transition State Theory may overestimate the rate because it requires more energy to overcome the barrier.&lt;br /&gt;
&lt;br /&gt;
=== Question 6. By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?  ===&lt;br /&gt;
[[File:12_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
As shown in the diagram above, it is a potential energy surfaces for F + H2 system. The LHS is for HF energy level which is lower than H2 energy level on the RHS. Because the F-H bond is stronger than H-H bond for &lt;br /&gt;
&lt;br /&gt;
F + H2 reaction is endothermic as stronger F-H bond formation required energy. Vice Versa, H + HF reaction is exothermic for strong H-F bond is broke.&lt;br /&gt;
&lt;br /&gt;
=== Question 7. Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
[[File:13_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Diagram above is the &#039;internuclear distance vs time&#039; for my estimated transition state structure.&lt;br /&gt;
&lt;br /&gt;
My best estimated transition state positions are F-H = 180.8 pm and H-H = 74.5 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Question 8. Report the activation energy for both reactions. ===&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;reaction, the activation energy is the energy differences between reactant and transition state structure. &lt;br /&gt;
&lt;br /&gt;
Ea=1.075 kJ/mol&lt;br /&gt;
&lt;br /&gt;
For H + HF reaction,&lt;br /&gt;
&lt;br /&gt;
Ea=126.682 kJ/mol&lt;br /&gt;
&lt;br /&gt;
=== Question 9. In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
[[File:14_01541238.png]][[File:15_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:16_01541238.png]][[File:17_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
For the F + H2 reaction. It is an exothermic reaction as the strong F-H bond formed. The potential energy will transfer to kinetic energy in order to complete the reaction. &lt;br /&gt;
&lt;br /&gt;
On diagram 1, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It shows that F-H bond is formed then break apart. Potential energy is transferred to kinetic energy that cause the recrossing &lt;br /&gt;
&lt;br /&gt;
barrier and go back to initial structure as the kinetic energy is too large. &lt;br /&gt;
&lt;br /&gt;
On diagram 2, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The diagram clearly shows 0.526 kJ kinetic energy is transferred which is lower than Activation energy and the reaction can&#039;t&lt;br /&gt;
&lt;br /&gt;
happen. F-H bond not formed.&lt;br /&gt;
&lt;br /&gt;
On diagram 3, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. F-H bond is formed after several formation and breakage. A significant amount of potential energy transfer into kinetic energy &lt;br /&gt;
&lt;br /&gt;
cause the oscillation for the middle H atom during the reaction.&lt;br /&gt;
&lt;br /&gt;
On diagram 4, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.6 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Kinetic energy is 1.707 kJ/mol overcomes the activation barrier and from the F-H bond.&lt;br /&gt;
&lt;br /&gt;
[[File:18_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
On the reverse reaction H + HF, the initial set is H-H = 230 pm and H-F = 100 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -20 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This diagram is one possible reactive trajectory for the reaction to complete. H atom carries 380.526 kJ/mol&lt;br /&gt;
&lt;br /&gt;
to collide with H-F molecule and form new H-H bond.&lt;br /&gt;
&lt;br /&gt;
In conclusion, the kinetic energy can be expressed as temperature. As the potential energy is transferred into kinetic energy, temperature will raise as the result of kinetic energy increases. Monitoring the temperature can help us&lt;br /&gt;
&lt;br /&gt;
to confirm this mechanism processes.&lt;br /&gt;
&lt;br /&gt;
=== Question 10. Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
Translational energy is due to the change in positions and states while vibrational energy is due to the change in structure of molecules. In fact, the translation energy is more effective in promoting reactions for system with early&lt;br /&gt;
&lt;br /&gt;
barrier, whereas vibrational energy is more effective for reactions with late barrier. The position of the transition state is at the top of the activation energy barrier curve on a energy-process diagram. As a result, if the transition state&lt;br /&gt;
&lt;br /&gt;
structure is similar to reactant (early barrier) translational energy is more effective. Vice Versa, if the transition state structure is more similar to the product (late barrier) vibrational energy is more effective. Moreover, symmetric &lt;br /&gt;
&lt;br /&gt;
structure always have higher reaction rate and reactivity than unsymmetric structure.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812771</id>
		<title>MRD:01541238</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812771"/>
		<updated>2020-06-04T18:53:51Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 2. Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= The Molecular reaction dynamics computational lab report =&lt;br /&gt;
&lt;br /&gt;
=== Question 1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
[[File:1.png]][[File:2.png]]&lt;br /&gt;
&lt;br /&gt;
These two diagrams are the counter plot and skew plot from a three H atoms model. A H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system.&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface diagram (gallery 2). The black reaction trajectory line shows the minimum energy path of the reactants to the products.&lt;br /&gt;
&lt;br /&gt;
When the trajectory line pass through the transition structure it shows a wavy line. And the transition state is defined as the maximum on the black trajectory minimum energy path.&lt;br /&gt;
&lt;br /&gt;
Mathematically the transition state point has the special property that ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 and the energy is higher than any other local minimum points on the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
And the transition state point is a critical point which can be identified by secondary derivative =0. The difference between local minimum is that they have a non zero second derivative number.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok but be careful with respect to what you mean by secondary derivative. You are looking for the secondary partial derivative of the reaction co ordinate with respect to the energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:49, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. ===&lt;br /&gt;
My best estimate of the transition state position &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;&#039;&#039;&#039;= 90.8 pm and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
According to the theory, when the structure is at transition structure, the trajectory point will only oscillate at on point.&lt;br /&gt;
&lt;br /&gt;
[[File:Dist vs time2.png]]&lt;br /&gt;
&lt;br /&gt;
The diagram above is the &#039;internuclear distance vs time&#039; plot for my best estimation of the positions. As shown on the diagram, there is almost no oscillation of the bond distances between B-C and A-B which means&lt;br /&gt;
&lt;br /&gt;
the structure is under a &#039;stable&#039; state and this structure is called transition state structure.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what did you use approximate this value?  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:53, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 3. Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ. ===&lt;br /&gt;
In my case, positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;91.8&#039;&#039;&#039; pm,  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;90.8 &#039;&#039;&#039;pm and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the new trajectory calculated.&lt;br /&gt;
&lt;br /&gt;
[[File:6_01541238.png]][[File:4_2_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Compare with two diagrams, the MEP doesn&#039;t have the vibrations of the atoms during the process while the trajectory shows oscillation to the products. And other remains the same, both direct to the same product.&lt;br /&gt;
&lt;br /&gt;
=== Question 4. Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ===&lt;br /&gt;
For the initial positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 74 pm and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 200 pm&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
7_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|unreactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
8_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Don&#039;t have enough energy to overcome the activation barrier, bounce&lt;br /&gt;
back to the more energy preferred state.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
9_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
10_2_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is much higher than the previous ones. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
twice and back to the initial conditions.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
11_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is higher than the previous one. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
three times and complete the reaction.&lt;br /&gt;
|}&lt;br /&gt;
The table above list some occasions for the different initial energies for the system. The table shows the energy is critically controlled in order to make the reaction complete.&lt;br /&gt;
&lt;br /&gt;
The total energy can&#039;t be too low so that can&#039;t pass though the energy barrier or too high to bounce back even through the transition state point twice. &lt;br /&gt;
&lt;br /&gt;
=== Question 5. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
With compare with experimental values, the Transition State Theory predictions will be over-estimated. Transition State Theory assumes the transition state structure will not go back to the initial reactants since the transition &lt;br /&gt;
&lt;br /&gt;
structure is formed. An equilibrium will form between the reactants and the transition states. However, in real life there is barrier recrossing cause the transition state structure goes back.&lt;br /&gt;
&lt;br /&gt;
Moreover, the Transition State Theory is treated classically Quantum mechanical effect like tunnelling effect is ignored. In real situations, particles with lower kinetic energy might able to cross the high energy barrier caused &lt;br /&gt;
&lt;br /&gt;
by tunnelling effect. Transition State Theory may overestimate the rate because it requires more energy to overcome the barrier.&lt;br /&gt;
&lt;br /&gt;
=== Question 6. By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?  ===&lt;br /&gt;
[[File:12_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
As shown in the diagram above, it is a potential energy surfaces for F + H2 system. The LHS is for HF energy level which is lower than H2 energy level on the RHS. Because the F-H bond is stronger than H-H bond for &lt;br /&gt;
&lt;br /&gt;
F + H2 reaction is endothermic as stronger F-H bond formation required energy. Vice Versa, H + HF reaction is exothermic for strong H-F bond is broke.&lt;br /&gt;
&lt;br /&gt;
=== Question 7. Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
[[File:13_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Diagram above is the &#039;internuclear distance vs time&#039; for my estimated transition state structure.&lt;br /&gt;
&lt;br /&gt;
My best estimated transition state positions are F-H = 180.8 pm and H-H = 74.5 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Question 8. Report the activation energy for both reactions. ===&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;reaction, the activation energy is the energy differences between reactant and transition state structure. &lt;br /&gt;
&lt;br /&gt;
Ea=1.075 kJ/mol&lt;br /&gt;
&lt;br /&gt;
For H + HF reaction,&lt;br /&gt;
&lt;br /&gt;
Ea=126.682 kJ/mol&lt;br /&gt;
&lt;br /&gt;
=== Question 9. In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
[[File:14_01541238.png]][[File:15_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:16_01541238.png]][[File:17_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
For the F + H2 reaction. It is an exothermic reaction as the strong F-H bond formed. The potential energy will transfer to kinetic energy in order to complete the reaction. &lt;br /&gt;
&lt;br /&gt;
On diagram 1, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It shows that F-H bond is formed then break apart. Potential energy is transferred to kinetic energy that cause the recrossing &lt;br /&gt;
&lt;br /&gt;
barrier and go back to initial structure as the kinetic energy is too large. &lt;br /&gt;
&lt;br /&gt;
On diagram 2, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The diagram clearly shows 0.526 kJ kinetic energy is transferred which is lower than Activation energy and the reaction can&#039;t&lt;br /&gt;
&lt;br /&gt;
happen. F-H bond not formed.&lt;br /&gt;
&lt;br /&gt;
On diagram 3, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. F-H bond is formed after several formation and breakage. A significant amount of potential energy transfer into kinetic energy &lt;br /&gt;
&lt;br /&gt;
cause the oscillation for the middle H atom during the reaction.&lt;br /&gt;
&lt;br /&gt;
On diagram 4, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.6 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Kinetic energy is 1.707 kJ/mol overcomes the activation barrier and from the F-H bond.&lt;br /&gt;
&lt;br /&gt;
[[File:18_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
On the reverse reaction H + HF, the initial set is H-H = 230 pm and H-F = 100 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -20 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This diagram is one possible reactive trajectory for the reaction to complete. H atom carries 380.526 kJ/mol&lt;br /&gt;
&lt;br /&gt;
to collide with H-F molecule and form new H-H bond.&lt;br /&gt;
&lt;br /&gt;
In conclusion, the kinetic energy can be expressed as temperature. As the potential energy is transferred into kinetic energy, temperature will raise as the result of kinetic energy increases. Monitoring the temperature can help us&lt;br /&gt;
&lt;br /&gt;
to confirm this mechanism processes.&lt;br /&gt;
&lt;br /&gt;
=== Question 10. Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
Translational energy is due to the change in positions and states while vibrational energy is due to the change in structure of molecules. In fact, the translation energy is more effective in promoting reactions for system with early&lt;br /&gt;
&lt;br /&gt;
barrier, whereas vibrational energy is more effective for reactions with late barrier. The position of the transition state is at the top of the activation energy barrier curve on a energy-process diagram. As a result, if the transition state&lt;br /&gt;
&lt;br /&gt;
structure is similar to reactant (early barrier) translational energy is more effective. Vice Versa, if the transition state structure is more similar to the product (late barrier) vibrational energy is more effective. Moreover, symmetric &lt;br /&gt;
&lt;br /&gt;
structure always have higher reaction rate and reactivity than unsymmetric structure.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812770</id>
		<title>MRD:01541238</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01541238&amp;diff=812770"/>
		<updated>2020-06-04T18:49:29Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= The Molecular reaction dynamics computational lab report =&lt;br /&gt;
&lt;br /&gt;
=== Question 1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
[[File:1.png]][[File:2.png]]&lt;br /&gt;
&lt;br /&gt;
These two diagrams are the counter plot and skew plot from a three H atoms model. A H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system.&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface diagram (gallery 2). The black reaction trajectory line shows the minimum energy path of the reactants to the products.&lt;br /&gt;
&lt;br /&gt;
When the trajectory line pass through the transition structure it shows a wavy line. And the transition state is defined as the maximum on the black trajectory minimum energy path.&lt;br /&gt;
&lt;br /&gt;
Mathematically the transition state point has the special property that ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 and the energy is higher than any other local minimum points on the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
And the transition state point is a critical point which can be identified by secondary derivative =0. The difference between local minimum is that they have a non zero second derivative number.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok but be careful with respect to what you mean by secondary derivative. You are looking for the secondary partial derivative of the reaction co ordinate with respect to the energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:49, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. ===&lt;br /&gt;
My best estimate of the transition state position &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;&#039;&#039;&#039;= 90.8 pm and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
According to the theory, when the structure is at transition structure, the trajectory point will only oscillate at on point.&lt;br /&gt;
&lt;br /&gt;
[[File:Dist vs time2.png]]&lt;br /&gt;
&lt;br /&gt;
The diagram above is the &#039;internuclear distance vs time&#039; plot for my best estimation of the positions. As shown on the diagram, there is almost no oscillation of the bond distances between B-C and A-B which means&lt;br /&gt;
&lt;br /&gt;
the structure is under a &#039;stable&#039; state and this structure is called transition state structure.&lt;br /&gt;
&lt;br /&gt;
=== Question 3. Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ. ===&lt;br /&gt;
In my case, positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;91.8&#039;&#039;&#039; pm,  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;90.8 &#039;&#039;&#039;pm and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the new trajectory calculated.&lt;br /&gt;
&lt;br /&gt;
[[File:6_01541238.png]][[File:4_2_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Compare with two diagrams, the MEP doesn&#039;t have the vibrations of the atoms during the process while the trajectory shows oscillation to the products. And other remains the same, both direct to the same product.&lt;br /&gt;
&lt;br /&gt;
=== Question 4. Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ===&lt;br /&gt;
For the initial positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 74 pm and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 200 pm&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
7_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|unreactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
8_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Don&#039;t have enough energy to overcome the activation barrier, bounce&lt;br /&gt;
back to the more energy preferred state.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
9_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
10_2_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is much higher than the previous ones. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
twice and back to the initial conditions.&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|reactive&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
11_01541238.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|Enough kinetic energy to overcome activation barrier.&lt;br /&gt;
The energy is higher than the previous one. &lt;br /&gt;
&lt;br /&gt;
Cause the reaction reacts back and overcomes the transition states &lt;br /&gt;
&lt;br /&gt;
three times and complete the reaction.&lt;br /&gt;
|}&lt;br /&gt;
The table above list some occasions for the different initial energies for the system. The table shows the energy is critically controlled in order to make the reaction complete.&lt;br /&gt;
&lt;br /&gt;
The total energy can&#039;t be too low so that can&#039;t pass though the energy barrier or too high to bounce back even through the transition state point twice. &lt;br /&gt;
&lt;br /&gt;
=== Question 5. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
With compare with experimental values, the Transition State Theory predictions will be over-estimated. Transition State Theory assumes the transition state structure will not go back to the initial reactants since the transition &lt;br /&gt;
&lt;br /&gt;
structure is formed. An equilibrium will form between the reactants and the transition states. However, in real life there is barrier recrossing cause the transition state structure goes back.&lt;br /&gt;
&lt;br /&gt;
Moreover, the Transition State Theory is treated classically Quantum mechanical effect like tunnelling effect is ignored. In real situations, particles with lower kinetic energy might able to cross the high energy barrier caused &lt;br /&gt;
&lt;br /&gt;
by tunnelling effect. Transition State Theory may overestimate the rate because it requires more energy to overcome the barrier.&lt;br /&gt;
&lt;br /&gt;
=== Question 6. By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?  ===&lt;br /&gt;
[[File:12_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
As shown in the diagram above, it is a potential energy surfaces for F + H2 system. The LHS is for HF energy level which is lower than H2 energy level on the RHS. Because the F-H bond is stronger than H-H bond for &lt;br /&gt;
&lt;br /&gt;
F + H2 reaction is endothermic as stronger F-H bond formation required energy. Vice Versa, H + HF reaction is exothermic for strong H-F bond is broke.&lt;br /&gt;
&lt;br /&gt;
=== Question 7. Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
[[File:13_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
Diagram above is the &#039;internuclear distance vs time&#039; for my estimated transition state structure.&lt;br /&gt;
&lt;br /&gt;
My best estimated transition state positions are F-H = 180.8 pm and H-H = 74.5 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Question 8. Report the activation energy for both reactions. ===&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;reaction, the activation energy is the energy differences between reactant and transition state structure. &lt;br /&gt;
&lt;br /&gt;
Ea=1.075 kJ/mol&lt;br /&gt;
&lt;br /&gt;
For H + HF reaction,&lt;br /&gt;
&lt;br /&gt;
Ea=126.682 kJ/mol&lt;br /&gt;
&lt;br /&gt;
=== Question 9. In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
[[File:14_01541238.png]][[File:15_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:16_01541238.png]][[File:17_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
For the F + H2 reaction. It is an exothermic reaction as the strong F-H bond formed. The potential energy will transfer to kinetic energy in order to complete the reaction. &lt;br /&gt;
&lt;br /&gt;
On diagram 1, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It shows that F-H bond is formed then break apart. Potential energy is transferred to kinetic energy that cause the recrossing &lt;br /&gt;
&lt;br /&gt;
barrier and go back to initial structure as the kinetic energy is too large. &lt;br /&gt;
&lt;br /&gt;
On diagram 2, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The diagram clearly shows 0.526 kJ kinetic energy is transferred which is lower than Activation energy and the reaction can&#039;t&lt;br /&gt;
&lt;br /&gt;
happen. F-H bond not formed.&lt;br /&gt;
&lt;br /&gt;
On diagram 3, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.0 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. F-H bond is formed after several formation and breakage. A significant amount of potential energy transfer into kinetic energy &lt;br /&gt;
&lt;br /&gt;
cause the oscillation for the middle H atom during the reaction.&lt;br /&gt;
&lt;br /&gt;
On diagram 4, the set is F-H = 230 pm and H-H = 74 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.6 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Kinetic energy is 1.707 kJ/mol overcomes the activation barrier and from the F-H bond.&lt;br /&gt;
&lt;br /&gt;
[[File:18_01541238.png]]&lt;br /&gt;
&lt;br /&gt;
On the reverse reaction H + HF, the initial set is H-H = 230 pm and H-F = 100 pm when &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -20 &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This diagram is one possible reactive trajectory for the reaction to complete. H atom carries 380.526 kJ/mol&lt;br /&gt;
&lt;br /&gt;
to collide with H-F molecule and form new H-H bond.&lt;br /&gt;
&lt;br /&gt;
In conclusion, the kinetic energy can be expressed as temperature. As the potential energy is transferred into kinetic energy, temperature will raise as the result of kinetic energy increases. Monitoring the temperature can help us&lt;br /&gt;
&lt;br /&gt;
to confirm this mechanism processes.&lt;br /&gt;
&lt;br /&gt;
=== Question 10. Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
Translational energy is due to the change in positions and states while vibrational energy is due to the change in structure of molecules. In fact, the translation energy is more effective in promoting reactions for system with early&lt;br /&gt;
&lt;br /&gt;
barrier, whereas vibrational energy is more effective for reactions with late barrier. The position of the transition state is at the top of the activation energy barrier curve on a energy-process diagram. As a result, if the transition state&lt;br /&gt;
&lt;br /&gt;
structure is similar to reactant (early barrier) translational energy is more effective. Vice Versa, if the transition state structure is more similar to the product (late barrier) vibrational energy is more effective. Moreover, symmetric &lt;br /&gt;
&lt;br /&gt;
structure always have higher reaction rate and reactivity than unsymmetric structure.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812769</id>
		<title>MRD:01547559</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812769"/>
		<updated>2020-06-04T18:36:49Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 5: Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Molecular Reaction Dynamics: Applications to triatomic systems- Poppy Tobolski==&lt;br /&gt;
&lt;br /&gt;
===&amp;lt;u&amp;gt;Exercise 1&amp;lt;/u&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
NOTE- r1= BC distance, r2= AB distance, p1= BC momentum, p2= AB momentum. However, it doesn&#039;t matter because this is a symmetrical system.&lt;br /&gt;
&lt;br /&gt;
==== Question 1: On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state resembles that of the reactants or products depending on which it is closer in energy to. In an exothermic reaction, the transition state is closer in energy to the reactants therefore, it resembles that of the reactants over the products. This is an early transition state. In an endothermic reaction the transition state is closer in energy to the products and so the transition state resembles that of the products. This is a late transition state. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|TGood introduction - a reference for Hammonds postulate may help here [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0,  it&#039;s the point where the gradient equals zero. The transition state is at the local maximum within the well of minima, the saddle point. In the surface plot, there is a minimum path that connects the products to the reactants. The transition state can be identified as it is the maxima in this path, this is shown in figure 1. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, the saddle is where the first partial derivative = 0 in both the reaction and orthogonal to the reaction co-ordinates. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
At the transition state, the H atoms do not move because force is a derivative of the potential energy. Therefore, force is zero and so the atoms are stationary.&lt;br /&gt;
&lt;br /&gt;
[[file:transitionstatemaximum_pt1118.png|300px|thumb|Figure 1-This graph is the surface plot for the reaction of H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. In this image, you can see there is a maximum is the minimum energy path, this shows the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|A second derivative will allow you to determine which direction the maxima and minima are in. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
rAB= rBC=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.77pm&lt;br /&gt;
&lt;br /&gt;
When the distance between each of the H atoms equals this the force along the distances is very close to zero. Force is a derivative of the potential energy, and so when it equals zero it means the nuclei in the transition state are zero. It can be seen in figure 2 that the internuclear distance isn&#039;t changing with time when at the transition state, this is because the atoms are stationary.&lt;br /&gt;
&lt;br /&gt;
[[file:forceequalszeropt1118.png|300px|thumb|left|Figure 2-This graph is of the internuclear distance vs time for the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Well described. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Question 3: Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
&lt;br /&gt;
When the MEP calculation is used the path is straight, however, when the dynamic calculation is used the path becomes curved. This is because the molecule is oscillating, but in the MEP calculation this is being ignored. The velocity is zero in the MEP calculation, so the path follows the minima on the valley floor of the product. The MEP calculation is not as realistic as the dynamic calculation, this is because it doesn&#039;t take into account that the atoms have masses and in MEP calculation the molecules have uniform motion. Figures 3 and 4 show this on a contour plot.&lt;br /&gt;
[[file:dynamicpt1118.png|thumb|200px|Figure 3- Contour plot of r1=rts+1 vs r2=rts, dynamic calculation has been used. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:meppt1118.png|thumb|200px|Figure 4- Contour plot of r1=rts+1 vs r2=rts, MEP calculation has been used. A is the approaching H atom and BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|I tihnk a little more information is required here on  the differences between MEP and dynamics. Good description regardless. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Look at the “Internuclear Distances vs Time” and “Momenta vs Time”. What would change if we used the initial conditions r1 = rts and r2 = rts+1 pm instead?&amp;lt;/b&amp;gt;&lt;br /&gt;
When looking at the internuclear distances vs time graph, when you swap r1 and r2 around, the graph follows the same trend except the lines for r1 and r2 change around. This is because now r1 decreases distance slightly as it becomes the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule with time and r2 increases distance with time as the H atom moves away. After about 15 seconds, the reaction has finished as r1 is just oscillating around the H-H bond distance and the other H atom has moved away fully. This is shown by figure 5 and 6. Again for the momenta vs time graph, when you change r1 and r2, the two lines in the graph follow the same trend but they are now swapped over. This is because now p2 increases over time and so the momentum of this H atom moving away increases faster and then plateaus once it has moved fully away and has no attraction to the molecule. For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule the momenta oscillates. This is shown by figure 7 and 8.&lt;br /&gt;
[[file:internuclear1pt1118.png|thumb|200px|Figure 5- Internuclear distance vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:internuclear2pt1118.png|thumb|200px|Figure 6- Internuclear distance vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta1pt1118.png|thumb|200px|Figure 7- Momenta vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta2pt1118.png|thumb|200px|Figure 8- Momenta vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed.&lt;br /&gt;
What do you observe?&amp;lt;/b&amp;gt;&lt;br /&gt;
To get the final positions the &#039;get last geometry&#039; function was used. The final r1=74.04pm, r2=352.59pm, p1=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2=-5.08g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Figures 9 and 10, show the internuclear distance vs time graph and the momenta vs time graph respectively. For the internuclear distance vs time graph the r1 distance increased to a maximum and the r2 distance decreased to a minimum over time. They increased and decreased to the distance at which the transition state is achieved so r1=r2=rts. For the momenta vs time graph, the p2 increased as the H atom approached the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and then reached zero when the transition state was reached again. It continued to increase again as the r2 distance increased again. p1 also increased but in an oscillating fashion, it plateaued when momenta was zero for a bit, when in the transition state, and then over time increased again after the transition state had passed.&lt;br /&gt;
[[file:finalinternuclearpt1118.png|thumb|200px|Figure 9- This is the internuclear distance vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
[[file:finalmomentapt1118.png|thumb|200px|Figure 10- This is the momenta vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
&lt;br /&gt;
====Question 4: Complete the table by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
&lt;br /&gt;
A is the approach H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! p1/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  p2/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 ||-414.280 ||Reactive||The black line shows the reaction dynamics, the AB distance decreases as A approaches BC. The BC distance increases, until the transition state is reached. The reaction occurs and so the transition state is past and AB molecule is formed as C moves away. The black line passes down the product energy valley. ||[[file:row1_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.077 ||no reaction||The black line shows that the AB distance decreases to get to the transition state however, the transition state can not be reached. This is because there&#039;s not enough kinetic energy to get to the transition state and so overcome the energy barrier and form the products and it goes back to the reactants. The black line curves round as A starts to move away from molecule BC again. ||[[file:row2_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1|| -413.977 ||reactive||This reaction dynamic is very similar to the first one. A approaches BC, the AB distance decreases and the BC distance slightly increases therefore, forming the transition state. There&#039;s enough kinetic energy and so the reaction occurs. AB molecule forms and the black line shows this as it travels down the valley of the product energy. ||[[file:row3_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1|| -357.277 ||no reaction  ||From looking at the black line it can be seen that A approaches BC and some interaction forms, the transition state is reached. C still has some attraction to B . B moves between A and C, but goes back to form a molecule with C. The p2 is not large enough for the reaction to continue to form the products. There is enough kinetic energy for the reaction to occur, however, not all this kinetic energy may be as translational energy which is important for the reaction to occur. It is instead vibrational energy of the BC molecule.||[[file:row4_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 ||-349.477 ||reactive ||It can be seen that A moves towards BC and BC distance becomes larger, eventually getting to the transition state. B moves back and forth between A and C forming molecules with both. Eventually, B gets closer to A and further from C and so forming AB molecule, this time p2 is large enough and so the reaction can occur. ||[[file:row5_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
To conclude, in order for a reaction to occur there needs to be enough kinetic energy. Enough of this kinetic energy needs to be translational energy, if all the kinetic energy is vibrational energy of the reactants molecule then the reaction won&#039;t occur. Reaction 1 and 3 show that when p1 is higher the reaction will occur faster. Lastly, p1 and p2 need to both be large enough in order for them to collide and for a reaction to occur as shown by the 4th and 5th set of conditions.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good descriptions in the table. Be careful with the descriptions with A / B / C etc as this can get a bit confusing. You have concluded the work well here. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:09, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Question 5: Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
&lt;br /&gt;
Transition state theory assumes that if the reactants have enough energy the transition state will be reached and it will go on to form the products. However, even if there&#039;s enough kinetic energy, then it doesn&#039;t always mean a reaction will occur. This is shown by experimental values. The energy has to be spread correctly, for example as translational energy and not just vibrational energy of the molecule. Therefore, this will decrease the experimental rate because not all the kinetic energy is used as translational energy for the reaction.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Transition state theory also assumes that once you go past the transition state and on to form the products that you cannot go back to form the reactants again. However, in experiment this is possible. Experiment 4 in the table above is an example of this, the reaction doesn&#039;t occur even though the transition state is reached. This also means the experimental rate is lower than predicted as not all the reactants will turn into products even if the transition state is reached.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good well answered. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
It also assumes that the reaction can be treated classically, but quantum effects do occur in experiment. For example quantum tunnelling, this increases the experimental rate compared to the prediction. &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state theory lastly assumes a quasi-equilibrium between the reactants and transition state.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; How much transition state you get is determined by how much reactant you have and so this determines how much product you will get. However, in experiment there may not be an equilibrium, and therefore, this would mean the experimental rate value would be higher than predicted.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|The experiment in this case is representative of one particular momenta combination of atom and molecule. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===&amp;lt;u&amp;gt;Exercise 2&amp;lt;/u&amp;gt;===&lt;br /&gt;
 &lt;br /&gt;
====Question 1/2: By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
A= F, B=H, C=H&lt;br /&gt;
&lt;br /&gt;
F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. This reaction is exothermic, the energy of the reactants are higher than that of the products. This is an exothermic reaction because it forms stronger bonds in the products than those which are in the reactants,  it forms HF which has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. More energy is released when the HF bond forms than is needed to break the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond. This also means the transition state will be more similar to the reactants, it is an early transition state. Therefore, the transition state is near to when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the reactant and the minimum pathway on the left (AB) is the product. Therefore, you can see the product energy is lower than the reactant energy and so it&#039;s exothermic.&lt;br /&gt;
The enthalpy change for this reaction is -129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
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{{fontcolor1|green| Good referencing the figure here.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:24, 4 June 2020 (BST)}}&lt;br /&gt;
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HF+H. This reaction is endothermic, the energy of the reactants are lower than that of the products. HF has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, therefore, energy needs to be put into the reaction to break this bond and so the reaction is endothermic. More energy is needed to break the HF bond than is released when the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond is formed. This means that the transition state will be more similar to the products, it is a late transition state. Therefore, the transition state is near when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the product and the minimum pathway on the left is the reactant. Therefore, you can see the reactant energy is higher than the product energy and so it&#039;s endothermic.&lt;br /&gt;
The enthalpy change for this reaction is 129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
&lt;br /&gt;
Both reactions have the same transition state as they are the same reactions just going in opposite directions. I found the transition by finding where the force equals zero and then checking using the internuclear distances vs time graph to see that the graph was zero. This can be seen in figure 11.&lt;br /&gt;
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{{fontcolor1|green|Make sure to name figures numerically as they are referenced in the text, here 11 follows from 12. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:24, 4 June 2020 (BST)}}&lt;br /&gt;
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[[file:HHFtspt1118.png|thumb|left|200px|Figure 11- Shows the internuclear distance vs time graph of the transition state of the HF + H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reactions]]&lt;br /&gt;
[[File:Screen Shot 2020-05-22 at 11.14.01.png|thumb|200px|Figure 12- This shows the surface plot for the reactions of H+HF and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F. AB distance is showing F approaching H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and BC distance is showing H approaching HF. AB is the distance between F and H and BC is the distance between H and H.]]&lt;br /&gt;
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====Question 3: Report the activation energy for both reactions.====&lt;br /&gt;
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The activation energy can be determined by taking away the energy of the reactants from the transition state energy.&lt;br /&gt;
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Using LEPS GUI and changing the distances of AB and BC, the energies for the H-F and H-H bonds can be determined. For the H-F bond energy I found to be -560.404 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is similar to -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; which it says in literature. To find this energy, I set the AB distance as 91pm and the BC distance as 4000pm so that the H atom (C) is so far away it doesn&#039;t give any interaction on the HF bond. For the H-H bond energy I found it to be -435.057 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, again this is close to the literature which was -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. To find this energy, I set the AB distance as 4000pm and the BC distance as 74.5pm. &lt;br /&gt;
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{{fontcolor1|green| Good description and compariing to literature.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:24, 4 June 2020 (BST)}}&lt;br /&gt;
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Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--435.057=1.076 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy of HF + H= -433.981--560.404=126.423 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy can also be determined using an MEP calculation and slightly displacing the transition state towards the reactants, this is a more accurate method because in the above method we are assuming that moving the atoms far apart will give us pure reactants.&lt;br /&gt;
&lt;br /&gt;
To determine activation energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the AB distance=182 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a very small drop in the graph and so using the initial and final energies the activation energy can be determined. Figure 13 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--434.144=0.163 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAEpt1118.png|thumb|200px|Figure 13- this shows the energy vs time graph used to calculate the activation energy for the reaction of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
&lt;br /&gt;
To determine activation energy of HF+H, the AB distance=180 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a drop in the graph and so using the two horizontal lines the activation energy can be determined. Figure 14 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of HF + H= -433.981--560.063= 126.082 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAE2pt1118.png|thumb|200px|Figure 14- this shows the energy vs time graph used to calculate the activation energy for the reaction of HF+F.]]&lt;br /&gt;
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Overall both methods give very similar values for the activation energies of the reactions.&lt;br /&gt;
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{{fontcolor1|green| Very well done, great answer and good comparison. You have made it really clear how you determined the energies in both cases and the calculations are sound. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:24, 4 June 2020 (BST)}}&lt;br /&gt;
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====Question 4: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;br /&gt;
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Reaction conditions for a reactive trajectory of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F are rHF= AB distance =180 pm, rHH= BC distance = 74 pm, pHF=AB momentum= -1.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and pHH= BC momentum= 0.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The number of steps is 3000. &lt;br /&gt;
&lt;br /&gt;
The energy is conserved, therefore, the potential energy is converted to kinetic energy. This can be seen by the increase in oscillation in figure 15, once the transition state has been overcome and products starting to form. A large amount of the total energy goes to being vibrational energy of the product.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; The product molecule is oscillating lots therefore, can see that this is vibrational energy. Translational energy directs it to get over the potential energy barrier and then it can drop down and the energy becomes vibrational kinetic energy.&lt;br /&gt;
&lt;br /&gt;
[[File:Reactiondynamicspt1118.png|thumb|200px|Figure 15- This is contour plot showing the reaction dynamics of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is BC and F is A.]]&lt;br /&gt;
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It can be confirmed experimentally as the reactants and products have different vibrational energy states, and so can be tested using IR spectroscopy. It can be checked by looking either at the emission or absorption of the molecules. &lt;br /&gt;
For the reactants all the molecules are in the ground state, when it forms the products some of the molecules are excited, therefore, the some of the products are in the ground state and some in the first excited state. &lt;br /&gt;
When looking at absorption, you can see for the reactants the molecules in the ground state will get excited to the first excited energy level. Therefore, there is only one transition and so there will be only one peak in the IR spectrum. For the products, two transitions can occur, the molecules in the ground state can be excited to the first excited energy level (fundamental transition), and the molecules that are already in the first excited state will be excited to the second excited state (this is an overtone). These two transitions absorb at two different wavelengths. The IR spectrum will now have the same peak as the reactants as well as a peak at a lower wavenumber. This second peak is at a lower wavenumber because the difference between the first and second state is smaller than the difference between the ground state and first excited state, this is due to the anharmonicity of the system. Overtime the intensity of this overtone will decrease and the intensity of the fundamental will increase as molecules fall back down to the ground state. For looking at emission, instead of the molecules being excited they will fall back to the ground state and so light is emitted. This time, the reactant IR will have no peaks as all molecules are already in the ground state. For the products, there will be one peak as the molecules in the first excited state drop back down to the ground state. &lt;br /&gt;
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Chemiluminescence experiments can be run to study these reactions.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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{{fontcolor1|green| Ok, I think you could have mentioned some other techniques away from IR [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:30, 4 June 2020 (BST)}}&lt;br /&gt;
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&amp;lt;b&amp;gt;Setup a calculation starting on the side of the reactants of F + H2, at the bottom of the well rHH = 74 pm, with a momentum pFH = -1.0 g.mol-1.pm.fs-1, and explore several values of pHH in the range -6.1 to 6.1 g.mol-1.pm.fs-1 (explore values also close to these limits). What do you observe? &amp;lt;/b&amp;gt;&lt;br /&gt;
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The initial  rHF distance= 230 pm. A=F B=H C=H&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! pHF/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  pHH/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -6.0 ||-404.014 ||reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule oscillates as it approaches the F atom. At a time when the H atoms in the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule are repelling one another, there is an interaction between the F atom and the H atom (B). The H atom (B) bounces to and fro between the H (C) and F atoms, eventually forms a HF molecule when the other H atom starts to move away. The products oscillate more than the reactants, therefore, they have more vibrational energy.||[[file:row11_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -4.5 || -418.264 ||no reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule moves towards the F atom. The H atom (B) moves towards the F atom and forms the transition state but this atom then bounces back forming H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and moving away. Therefore, the energy barrier is not quite overcome as it rolls back to the reactants.||[[file:row22_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -2.0|| -432.014 ||no reaction||The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule starts to approach the F atom but there is not enough kinetic energy which is vibrational and in the correct direction for the transition state to be reached. The potential energy barrier can not be over come and so it rolls back to the reactants and no reaction occurs.||[[file:row33_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 2.0|| -428.014||no reaction ||This has the same trajectory as above except the molecules have a bit more vibrational energy as it oscillates a bit more. Again there&#039;s still not enough vibrational kinetic energy for the reactants to get over the potential energy barrier and a reaction to occur.||[[file:row44_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 6.0 ||-349.477 ||no reaction || The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; moves towards the F atom and the transition state is achieved. However, no reaction occurs and the molecules roll back to the reactants as opposed to the products. When the transition state is reached the H atom (B) bounces straight back to form the reactants again.||[[file:row55_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
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{{fontcolor1|green|The trajectories show the incoming atom to the molecule, not vice versa.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:30, 4 June 2020 (BST)}}&lt;br /&gt;
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&amp;lt;b&amp;gt;For the same initial position, increase slightly the momentum pFH = -1.6 g.mol-1.pm.fs-1, and considerably reduce the overall energy of the system by reducing the momentum pHH = 0.2 g.mol-1.pm.fs-1. What do you observe now?&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[file:figure16pt1118.png|thumb|200px|Figure 16- This shows the trajectory for the reaction that occurs between H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and F atom, when pBC= pHH = 0.2 g.mol-1.pm.fs-1 and pAB= pFH = -1.6 g.mol-1.pm.fs-1. BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and A is the F atom. ]]&lt;br /&gt;
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The reaction occurs. The vibrational energy of the products is much greater than that of the reactants, this can be seen in figure 16. This can be seen because the molecules in the product well oscillate more than the molecules in the reactant well. A lot of the potential energy has been converted to vibrational energy. The kinetic energy for this reaction is very low but, the amount of this that is vibrational is enough and in the correct direction in order for the reaction to occur. In this reaction the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F, the transition state is reached. H atom. (B) bounces between the F atom and H atom (C), eventually the H atom (C) moves away and the HF molecule forms.&lt;br /&gt;
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====Question 5: Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ====&lt;br /&gt;
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Polyani&#039;s rule is that vibrational energy is able to promote an endothermic reaction more efficiently than translational energy. This is because in an endothermic reaction it is a late transition state and so if translational energy is used to promote the reaction, then it will hit the potential energy barrier and bounce back, the products are higher in energy and so it can not be used to direct to them. Energy needs to be put in to get over the energy barrier. Using translational energy means the incoming atom will hit the molecule and just bounce back, it can&#039;t get over the energy barrier. This energy is not in the correct direction for a reaction to occur. If vibrational energy is used then the molecule will be oscillating in the correct direction for a reaction to take place and can pass over the energy barrier. Therefore, the vibrational energy is more efficient at promoting an endothermic reaction.&lt;br /&gt;
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In an exothermic reaction, translational energy is more efficient than vibrational energy, it has an early transition state. This is because the energy is going down hill. The molecule can now move along the potential energy surface and once it gets to the transition state it can be guided around and move along in the correct direction to form the products. The translational energy directs the reactants to the products. In an exothermic reaction, the transition state is early and so the activation energy is much lower and so easier to get over the potential energy barrier, no energy needs to be put into the system. Therefore, it can just roll down using translational energy and so translational energy is more efficient for this reaction over vibrational energy. For an exothermic reaction, the energy is mainly changed from the translational energy to the vibrational energy of the products.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Ok, am not sure if you are referring diretly to your table of results here. You have described Polanyis rules but have not grounded them within the F-H-H system. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:36, 4 June 2020 (BST)}}&lt;br /&gt;
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== References==&lt;br /&gt;
1. K. J. Laidler. Chemical Kinetics. 3rd edition. Harper Collins. 1987&lt;br /&gt;
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2. Ch301.cm.utexas.edu. 2020. Bond Enthalpies. [online] Available at: &amp;lt;https://ch301.cm.utexas.edu/section2.php?target=thermo/thermochemistry/enthalpy-bonds.html&amp;gt; [Accessed 21 May 2020].&lt;br /&gt;
&lt;br /&gt;
3. Chemistry LibreTexts. 2020. Bond Energies. [online] Available at:&amp;lt;https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Supplemental_Modules_(Physical_and_Theoretical_Chemistry)/Chemical_Bonding/Fundamentals_of_Chemical_Bonding/Bond_Energies&amp;gt; [Accessed 21 May 2020].&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812768</id>
		<title>MRD:01547559</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812768"/>
		<updated>2020-06-04T18:30:37Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 4: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally. */&lt;/p&gt;
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&lt;div&gt;== Molecular Reaction Dynamics: Applications to triatomic systems- Poppy Tobolski==&lt;br /&gt;
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===&amp;lt;u&amp;gt;Exercise 1&amp;lt;/u&amp;gt;===&lt;br /&gt;
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NOTE- r1= BC distance, r2= AB distance, p1= BC momentum, p2= AB momentum. However, it doesn&#039;t matter because this is a symmetrical system.&lt;br /&gt;
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==== Question 1: On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state resembles that of the reactants or products depending on which it is closer in energy to. In an exothermic reaction, the transition state is closer in energy to the reactants therefore, it resembles that of the reactants over the products. This is an early transition state. In an endothermic reaction the transition state is closer in energy to the products and so the transition state resembles that of the products. This is a late transition state. &lt;br /&gt;
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{{fontcolor1|green|TGood introduction - a reference for Hammonds postulate may help here [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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The transition state is mathematically defined as ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0,  it&#039;s the point where the gradient equals zero. The transition state is at the local maximum within the well of minima, the saddle point. In the surface plot, there is a minimum path that connects the products to the reactants. The transition state can be identified as it is the maxima in this path, this is shown in figure 1. &lt;br /&gt;
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{{fontcolor1|green|Ok, the saddle is where the first partial derivative = 0 in both the reaction and orthogonal to the reaction co-ordinates. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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At the transition state, the H atoms do not move because force is a derivative of the potential energy. Therefore, force is zero and so the atoms are stationary.&lt;br /&gt;
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[[file:transitionstatemaximum_pt1118.png|300px|thumb|Figure 1-This graph is the surface plot for the reaction of H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. In this image, you can see there is a maximum is the minimum energy path, this shows the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
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{{fontcolor1|green|A second derivative will allow you to determine which direction the maxima and minima are in. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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==== Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
rAB= rBC=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.77pm&lt;br /&gt;
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When the distance between each of the H atoms equals this the force along the distances is very close to zero. Force is a derivative of the potential energy, and so when it equals zero it means the nuclei in the transition state are zero. It can be seen in figure 2 that the internuclear distance isn&#039;t changing with time when at the transition state, this is because the atoms are stationary.&lt;br /&gt;
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[[file:forceequalszeropt1118.png|300px|thumb|left|Figure 2-This graph is of the internuclear distance vs time for the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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{{fontcolor1|green|Well described. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:02, 4 June 2020 (BST)}}&lt;br /&gt;
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==== Question 3: Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
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When the MEP calculation is used the path is straight, however, when the dynamic calculation is used the path becomes curved. This is because the molecule is oscillating, but in the MEP calculation this is being ignored. The velocity is zero in the MEP calculation, so the path follows the minima on the valley floor of the product. The MEP calculation is not as realistic as the dynamic calculation, this is because it doesn&#039;t take into account that the atoms have masses and in MEP calculation the molecules have uniform motion. Figures 3 and 4 show this on a contour plot.&lt;br /&gt;
[[file:dynamicpt1118.png|thumb|200px|Figure 3- Contour plot of r1=rts+1 vs r2=rts, dynamic calculation has been used. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:meppt1118.png|thumb|200px|Figure 4- Contour plot of r1=rts+1 vs r2=rts, MEP calculation has been used. A is the approaching H atom and BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
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{{fontcolor1|green|I tihnk a little more information is required here on  the differences between MEP and dynamics. Good description regardless. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:04, 4 June 2020 (BST)}}&lt;br /&gt;
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&amp;lt;b&amp;gt;Look at the “Internuclear Distances vs Time” and “Momenta vs Time”. What would change if we used the initial conditions r1 = rts and r2 = rts+1 pm instead?&amp;lt;/b&amp;gt;&lt;br /&gt;
When looking at the internuclear distances vs time graph, when you swap r1 and r2 around, the graph follows the same trend except the lines for r1 and r2 change around. This is because now r1 decreases distance slightly as it becomes the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule with time and r2 increases distance with time as the H atom moves away. After about 15 seconds, the reaction has finished as r1 is just oscillating around the H-H bond distance and the other H atom has moved away fully. This is shown by figure 5 and 6. Again for the momenta vs time graph, when you change r1 and r2, the two lines in the graph follow the same trend but they are now swapped over. This is because now p2 increases over time and so the momentum of this H atom moving away increases faster and then plateaus once it has moved fully away and has no attraction to the molecule. For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule the momenta oscillates. This is shown by figure 7 and 8.&lt;br /&gt;
[[file:internuclear1pt1118.png|thumb|200px|Figure 5- Internuclear distance vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:internuclear2pt1118.png|thumb|200px|Figure 6- Internuclear distance vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta1pt1118.png|thumb|200px|Figure 7- Momenta vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta2pt1118.png|thumb|200px|Figure 8- Momenta vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed.&lt;br /&gt;
What do you observe?&amp;lt;/b&amp;gt;&lt;br /&gt;
To get the final positions the &#039;get last geometry&#039; function was used. The final r1=74.04pm, r2=352.59pm, p1=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2=-5.08g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Figures 9 and 10, show the internuclear distance vs time graph and the momenta vs time graph respectively. For the internuclear distance vs time graph the r1 distance increased to a maximum and the r2 distance decreased to a minimum over time. They increased and decreased to the distance at which the transition state is achieved so r1=r2=rts. For the momenta vs time graph, the p2 increased as the H atom approached the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and then reached zero when the transition state was reached again. It continued to increase again as the r2 distance increased again. p1 also increased but in an oscillating fashion, it plateaued when momenta was zero for a bit, when in the transition state, and then over time increased again after the transition state had passed.&lt;br /&gt;
[[file:finalinternuclearpt1118.png|thumb|200px|Figure 9- This is the internuclear distance vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
[[file:finalmomentapt1118.png|thumb|200px|Figure 10- This is the momenta vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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====Question 4: Complete the table by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
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A is the approach H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! p1/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  p2/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
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| -2.56 || -5.1 ||-414.280 ||Reactive||The black line shows the reaction dynamics, the AB distance decreases as A approaches BC. The BC distance increases, until the transition state is reached. The reaction occurs and so the transition state is past and AB molecule is formed as C moves away. The black line passes down the product energy valley. ||[[file:row1_pt1118.png|200px]]&lt;br /&gt;
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| -3.1 || -4.1 || -420.077 ||no reaction||The black line shows that the AB distance decreases to get to the transition state however, the transition state can not be reached. This is because there&#039;s not enough kinetic energy to get to the transition state and so overcome the energy barrier and form the products and it goes back to the reactants. The black line curves round as A starts to move away from molecule BC again. ||[[file:row2_pt1118.png|200px]]&lt;br /&gt;
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| -3.1 || -5.1|| -413.977 ||reactive||This reaction dynamic is very similar to the first one. A approaches BC, the AB distance decreases and the BC distance slightly increases therefore, forming the transition state. There&#039;s enough kinetic energy and so the reaction occurs. AB molecule forms and the black line shows this as it travels down the valley of the product energy. ||[[file:row3_pt1118.png|200px]]&lt;br /&gt;
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| -5.1 || -10.1|| -357.277 ||no reaction  ||From looking at the black line it can be seen that A approaches BC and some interaction forms, the transition state is reached. C still has some attraction to B . B moves between A and C, but goes back to form a molecule with C. The p2 is not large enough for the reaction to continue to form the products. There is enough kinetic energy for the reaction to occur, however, not all this kinetic energy may be as translational energy which is important for the reaction to occur. It is instead vibrational energy of the BC molecule.||[[file:row4_pt1118.png|200px]] &lt;br /&gt;
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| -5.1 || -10.6 ||-349.477 ||reactive ||It can be seen that A moves towards BC and BC distance becomes larger, eventually getting to the transition state. B moves back and forth between A and C forming molecules with both. Eventually, B gets closer to A and further from C and so forming AB molecule, this time p2 is large enough and so the reaction can occur. ||[[file:row5_pt1118.png|200px]] &lt;br /&gt;
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To conclude, in order for a reaction to occur there needs to be enough kinetic energy. Enough of this kinetic energy needs to be translational energy, if all the kinetic energy is vibrational energy of the reactants molecule then the reaction won&#039;t occur. Reaction 1 and 3 show that when p1 is higher the reaction will occur faster. Lastly, p1 and p2 need to both be large enough in order for them to collide and for a reaction to occur as shown by the 4th and 5th set of conditions.&lt;br /&gt;
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{{fontcolor1|green|Good descriptions in the table. Be careful with the descriptions with A / B / C etc as this can get a bit confusing. You have concluded the work well here. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:09, 4 June 2020 (BST)}}&lt;br /&gt;
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====Question 5: Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
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Transition state theory assumes that if the reactants have enough energy the transition state will be reached and it will go on to form the products. However, even if there&#039;s enough kinetic energy, then it doesn&#039;t always mean a reaction will occur. This is shown by experimental values. The energy has to be spread correctly, for example as translational energy and not just vibrational energy of the molecule. Therefore, this will decrease the experimental rate because not all the kinetic energy is used as translational energy for the reaction.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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Transition state theory also assumes that once you go past the transition state and on to form the products that you cannot go back to form the reactants again. However, in experiment this is possible. Experiment 4 in the table above is an example of this, the reaction doesn&#039;t occur even though the transition state is reached. This also means the experimental rate is lower than predicted as not all the reactants will turn into products even if the transition state is reached.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; &lt;br /&gt;
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{{fontcolor1|green| Good well answered. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:13, 4 June 2020 (BST)}}&lt;br /&gt;
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It also assumes that the reaction can be treated classically, but quantum effects do occur in experiment. For example quantum tunnelling, this increases the experimental rate compared to the prediction. &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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The transition state theory lastly assumes a quasi-equilibrium between the reactants and transition state.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; How much transition state you get is determined by how much reactant you have and so this determines how much product you will get. However, in experiment there may not be an equilibrium, and therefore, this would mean the experimental rate value would be higher than predicted.&lt;br /&gt;
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{{fontcolor1|green|The experiment in this case is representative of one particular momenta combination of atom and molecule. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:13, 4 June 2020 (BST)}}&lt;br /&gt;
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===&amp;lt;u&amp;gt;Exercise 2&amp;lt;/u&amp;gt;===&lt;br /&gt;
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====Question 1/2: By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? Locate the approximate position of the transition state.====&lt;br /&gt;
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A= F, B=H, C=H&lt;br /&gt;
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F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. This reaction is exothermic, the energy of the reactants are higher than that of the products. This is an exothermic reaction because it forms stronger bonds in the products than those which are in the reactants,  it forms HF which has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. More energy is released when the HF bond forms than is needed to break the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond. This also means the transition state will be more similar to the reactants, it is an early transition state. Therefore, the transition state is near to when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the reactant and the minimum pathway on the left (AB) is the product. Therefore, you can see the product energy is lower than the reactant energy and so it&#039;s exothermic.&lt;br /&gt;
The enthalpy change for this reaction is -129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
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{{fontcolor1|green| Good referencing the figure here.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:24, 4 June 2020 (BST)}}&lt;br /&gt;
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HF+H. This reaction is endothermic, the energy of the reactants are lower than that of the products. HF has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, therefore, energy needs to be put into the reaction to break this bond and so the reaction is endothermic. More energy is needed to break the HF bond than is released when the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond is formed. This means that the transition state will be more similar to the products, it is a late transition state. Therefore, the transition state is near when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the product and the minimum pathway on the left is the reactant. Therefore, you can see the reactant energy is higher than the product energy and so it&#039;s endothermic.&lt;br /&gt;
The enthalpy change for this reaction is 129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
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Both reactions have the same transition state as they are the same reactions just going in opposite directions. I found the transition by finding where the force equals zero and then checking using the internuclear distances vs time graph to see that the graph was zero. This can be seen in figure 11.&lt;br /&gt;
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{{fontcolor1|green|Make sure to name figures numerically as they are referenced in the text, here 11 follows from 12. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:24, 4 June 2020 (BST)}}&lt;br /&gt;
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[[file:HHFtspt1118.png|thumb|left|200px|Figure 11- Shows the internuclear distance vs time graph of the transition state of the HF + H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reactions]]&lt;br /&gt;
[[File:Screen Shot 2020-05-22 at 11.14.01.png|thumb|200px|Figure 12- This shows the surface plot for the reactions of H+HF and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F. AB distance is showing F approaching H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and BC distance is showing H approaching HF. AB is the distance between F and H and BC is the distance between H and H.]]&lt;br /&gt;
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====Question 3: Report the activation energy for both reactions.====&lt;br /&gt;
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The activation energy can be determined by taking away the energy of the reactants from the transition state energy.&lt;br /&gt;
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Using LEPS GUI and changing the distances of AB and BC, the energies for the H-F and H-H bonds can be determined. For the H-F bond energy I found to be -560.404 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is similar to -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; which it says in literature. To find this energy, I set the AB distance as 91pm and the BC distance as 4000pm so that the H atom (C) is so far away it doesn&#039;t give any interaction on the HF bond. For the H-H bond energy I found it to be -435.057 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, again this is close to the literature which was -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. To find this energy, I set the AB distance as 4000pm and the BC distance as 74.5pm. &lt;br /&gt;
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{{fontcolor1|green| Good description and compariing to literature.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:24, 4 June 2020 (BST)}}&lt;br /&gt;
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Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--435.057=1.076 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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Activation energy of HF + H= -433.981--560.404=126.423 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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The activation energy can also be determined using an MEP calculation and slightly displacing the transition state towards the reactants, this is a more accurate method because in the above method we are assuming that moving the atoms far apart will give us pure reactants.&lt;br /&gt;
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To determine activation energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the AB distance=182 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a very small drop in the graph and so using the initial and final energies the activation energy can be determined. Figure 13 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--434.144=0.163 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAEpt1118.png|thumb|200px|Figure 13- this shows the energy vs time graph used to calculate the activation energy for the reaction of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
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To determine activation energy of HF+H, the AB distance=180 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a drop in the graph and so using the two horizontal lines the activation energy can be determined. Figure 14 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of HF + H= -433.981--560.063= 126.082 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAE2pt1118.png|thumb|200px|Figure 14- this shows the energy vs time graph used to calculate the activation energy for the reaction of HF+F.]]&lt;br /&gt;
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Overall both methods give very similar values for the activation energies of the reactions.&lt;br /&gt;
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{{fontcolor1|green| Very well done, great answer and good comparison. You have made it really clear how you determined the energies in both cases and the calculations are sound. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:24, 4 June 2020 (BST)}}&lt;br /&gt;
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====Question 4: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;br /&gt;
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Reaction conditions for a reactive trajectory of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F are rHF= AB distance =180 pm, rHH= BC distance = 74 pm, pHF=AB momentum= -1.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and pHH= BC momentum= 0.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The number of steps is 3000. &lt;br /&gt;
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The energy is conserved, therefore, the potential energy is converted to kinetic energy. This can be seen by the increase in oscillation in figure 15, once the transition state has been overcome and products starting to form. A large amount of the total energy goes to being vibrational energy of the product.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; The product molecule is oscillating lots therefore, can see that this is vibrational energy. Translational energy directs it to get over the potential energy barrier and then it can drop down and the energy becomes vibrational kinetic energy.&lt;br /&gt;
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[[File:Reactiondynamicspt1118.png|thumb|200px|Figure 15- This is contour plot showing the reaction dynamics of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is BC and F is A.]]&lt;br /&gt;
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It can be confirmed experimentally as the reactants and products have different vibrational energy states, and so can be tested using IR spectroscopy. It can be checked by looking either at the emission or absorption of the molecules. &lt;br /&gt;
For the reactants all the molecules are in the ground state, when it forms the products some of the molecules are excited, therefore, the some of the products are in the ground state and some in the first excited state. &lt;br /&gt;
When looking at absorption, you can see for the reactants the molecules in the ground state will get excited to the first excited energy level. Therefore, there is only one transition and so there will be only one peak in the IR spectrum. For the products, two transitions can occur, the molecules in the ground state can be excited to the first excited energy level (fundamental transition), and the molecules that are already in the first excited state will be excited to the second excited state (this is an overtone). These two transitions absorb at two different wavelengths. The IR spectrum will now have the same peak as the reactants as well as a peak at a lower wavenumber. This second peak is at a lower wavenumber because the difference between the first and second state is smaller than the difference between the ground state and first excited state, this is due to the anharmonicity of the system. Overtime the intensity of this overtone will decrease and the intensity of the fundamental will increase as molecules fall back down to the ground state. For looking at emission, instead of the molecules being excited they will fall back to the ground state and so light is emitted. This time, the reactant IR will have no peaks as all molecules are already in the ground state. For the products, there will be one peak as the molecules in the first excited state drop back down to the ground state. &lt;br /&gt;
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Chemiluminescence experiments can be run to study these reactions.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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{{fontcolor1|green| Ok, I think you could have mentioned some other techniques away from IR [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:30, 4 June 2020 (BST)}}&lt;br /&gt;
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&amp;lt;b&amp;gt;Setup a calculation starting on the side of the reactants of F + H2, at the bottom of the well rHH = 74 pm, with a momentum pFH = -1.0 g.mol-1.pm.fs-1, and explore several values of pHH in the range -6.1 to 6.1 g.mol-1.pm.fs-1 (explore values also close to these limits). What do you observe? &amp;lt;/b&amp;gt;&lt;br /&gt;
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The initial  rHF distance= 230 pm. A=F B=H C=H&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! pHF/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  pHH/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -6.0 ||-404.014 ||reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule oscillates as it approaches the F atom. At a time when the H atoms in the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule are repelling one another, there is an interaction between the F atom and the H atom (B). The H atom (B) bounces to and fro between the H (C) and F atoms, eventually forms a HF molecule when the other H atom starts to move away. The products oscillate more than the reactants, therefore, they have more vibrational energy.||[[file:row11_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -4.5 || -418.264 ||no reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule moves towards the F atom. The H atom (B) moves towards the F atom and forms the transition state but this atom then bounces back forming H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and moving away. Therefore, the energy barrier is not quite overcome as it rolls back to the reactants.||[[file:row22_pt1118.png|200px]]&lt;br /&gt;
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| -1.0 || -2.0|| -432.014 ||no reaction||The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule starts to approach the F atom but there is not enough kinetic energy which is vibrational and in the correct direction for the transition state to be reached. The potential energy barrier can not be over come and so it rolls back to the reactants and no reaction occurs.||[[file:row33_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 2.0|| -428.014||no reaction ||This has the same trajectory as above except the molecules have a bit more vibrational energy as it oscillates a bit more. Again there&#039;s still not enough vibrational kinetic energy for the reactants to get over the potential energy barrier and a reaction to occur.||[[file:row44_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 6.0 ||-349.477 ||no reaction || The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; moves towards the F atom and the transition state is achieved. However, no reaction occurs and the molecules roll back to the reactants as opposed to the products. When the transition state is reached the H atom (B) bounces straight back to form the reactants again.||[[file:row55_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
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{{fontcolor1|green|The trajectories show the incoming atom to the molecule, not vice versa.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:30, 4 June 2020 (BST)}}&lt;br /&gt;
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&amp;lt;b&amp;gt;For the same initial position, increase slightly the momentum pFH = -1.6 g.mol-1.pm.fs-1, and considerably reduce the overall energy of the system by reducing the momentum pHH = 0.2 g.mol-1.pm.fs-1. What do you observe now?&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[file:figure16pt1118.png|thumb|200px|Figure 16- This shows the trajectory for the reaction that occurs between H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and F atom, when pBC= pHH = 0.2 g.mol-1.pm.fs-1 and pAB= pFH = -1.6 g.mol-1.pm.fs-1. BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and A is the F atom. ]]&lt;br /&gt;
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The reaction occurs. The vibrational energy of the products is much greater than that of the reactants, this can be seen in figure 16. This can be seen because the molecules in the product well oscillate more than the molecules in the reactant well. A lot of the potential energy has been converted to vibrational energy. The kinetic energy for this reaction is very low but, the amount of this that is vibrational is enough and in the correct direction in order for the reaction to occur. In this reaction the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F, the transition state is reached. H atom. (B) bounces between the F atom and H atom (C), eventually the H atom (C) moves away and the HF molecule forms.&lt;br /&gt;
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====Question 5: Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ====&lt;br /&gt;
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Polyani&#039;s rule is that vibrational energy is able to promote an endothermic reaction more efficiently than translational energy. This is because in an endothermic reaction it is a late transition state and so if translational energy is used to promote the reaction, then it will hit the potential energy barrier and bounce back, the products are higher in energy and so it can not be used to direct to them. Energy needs to be put in to get over the energy barrier. Using translational energy means the incoming atom will hit the molecule and just bounce back, it can&#039;t get over the energy barrier. This energy is not in the correct direction for a reaction to occur. If vibrational energy is used then the molecule will be oscillating in the correct direction for a reaction to take place and can pass over the energy barrier. Therefore, the vibrational energy is more efficient at promoting an endothermic reaction.&lt;br /&gt;
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In an exothermic reaction, translational energy is more efficient than vibrational energy, it has an early transition state. This is because the energy is going down hill. The molecule can now move along the potential energy surface and once it gets to the transition state it can be guided around and move along in the correct direction to form the products. The translational energy directs the reactants to the products. In an exothermic reaction, the transition state is early and so the activation energy is much lower and so easier to get over the potential energy barrier, no energy needs to be put into the system. Therefore, it can just roll down using translational energy and so translational energy is more efficient for this reaction over vibrational energy. For an exothermic reaction, the energy is mainly changed from the translational energy to the vibrational energy of the products.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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== References==&lt;br /&gt;
1. K. J. Laidler. Chemical Kinetics. 3rd edition. Harper Collins. 1987&lt;br /&gt;
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2. Ch301.cm.utexas.edu. 2020. Bond Enthalpies. [online] Available at: &amp;lt;https://ch301.cm.utexas.edu/section2.php?target=thermo/thermochemistry/enthalpy-bonds.html&amp;gt; [Accessed 21 May 2020].&lt;br /&gt;
&lt;br /&gt;
3. Chemistry LibreTexts. 2020. Bond Energies. [online] Available at:&amp;lt;https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Supplemental_Modules_(Physical_and_Theoretical_Chemistry)/Chemical_Bonding/Fundamentals_of_Chemical_Bonding/Bond_Energies&amp;gt; [Accessed 21 May 2020].&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812767</id>
		<title>MRD:01547559</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812767"/>
		<updated>2020-06-04T18:24:35Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Exercise 2 */&lt;/p&gt;
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&lt;div&gt;== Molecular Reaction Dynamics: Applications to triatomic systems- Poppy Tobolski==&lt;br /&gt;
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===&amp;lt;u&amp;gt;Exercise 1&amp;lt;/u&amp;gt;===&lt;br /&gt;
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NOTE- r1= BC distance, r2= AB distance, p1= BC momentum, p2= AB momentum. However, it doesn&#039;t matter because this is a symmetrical system.&lt;br /&gt;
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==== Question 1: On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state resembles that of the reactants or products depending on which it is closer in energy to. In an exothermic reaction, the transition state is closer in energy to the reactants therefore, it resembles that of the reactants over the products. This is an early transition state. In an endothermic reaction the transition state is closer in energy to the products and so the transition state resembles that of the products. This is a late transition state. &lt;br /&gt;
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{{fontcolor1|green|TGood introduction - a reference for Hammonds postulate may help here [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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The transition state is mathematically defined as ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0,  it&#039;s the point where the gradient equals zero. The transition state is at the local maximum within the well of minima, the saddle point. In the surface plot, there is a minimum path that connects the products to the reactants. The transition state can be identified as it is the maxima in this path, this is shown in figure 1. &lt;br /&gt;
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{{fontcolor1|green|Ok, the saddle is where the first partial derivative = 0 in both the reaction and orthogonal to the reaction co-ordinates. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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At the transition state, the H atoms do not move because force is a derivative of the potential energy. Therefore, force is zero and so the atoms are stationary.&lt;br /&gt;
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[[file:transitionstatemaximum_pt1118.png|300px|thumb|Figure 1-This graph is the surface plot for the reaction of H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. In this image, you can see there is a maximum is the minimum energy path, this shows the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
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{{fontcolor1|green|A second derivative will allow you to determine which direction the maxima and minima are in. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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==== Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
rAB= rBC=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.77pm&lt;br /&gt;
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When the distance between each of the H atoms equals this the force along the distances is very close to zero. Force is a derivative of the potential energy, and so when it equals zero it means the nuclei in the transition state are zero. It can be seen in figure 2 that the internuclear distance isn&#039;t changing with time when at the transition state, this is because the atoms are stationary.&lt;br /&gt;
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[[file:forceequalszeropt1118.png|300px|thumb|left|Figure 2-This graph is of the internuclear distance vs time for the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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{{fontcolor1|green|Well described. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:02, 4 June 2020 (BST)}}&lt;br /&gt;
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==== Question 3: Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
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When the MEP calculation is used the path is straight, however, when the dynamic calculation is used the path becomes curved. This is because the molecule is oscillating, but in the MEP calculation this is being ignored. The velocity is zero in the MEP calculation, so the path follows the minima on the valley floor of the product. The MEP calculation is not as realistic as the dynamic calculation, this is because it doesn&#039;t take into account that the atoms have masses and in MEP calculation the molecules have uniform motion. Figures 3 and 4 show this on a contour plot.&lt;br /&gt;
[[file:dynamicpt1118.png|thumb|200px|Figure 3- Contour plot of r1=rts+1 vs r2=rts, dynamic calculation has been used. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:meppt1118.png|thumb|200px|Figure 4- Contour plot of r1=rts+1 vs r2=rts, MEP calculation has been used. A is the approaching H atom and BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
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{{fontcolor1|green|I tihnk a little more information is required here on  the differences between MEP and dynamics. Good description regardless. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:04, 4 June 2020 (BST)}}&lt;br /&gt;
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&amp;lt;b&amp;gt;Look at the “Internuclear Distances vs Time” and “Momenta vs Time”. What would change if we used the initial conditions r1 = rts and r2 = rts+1 pm instead?&amp;lt;/b&amp;gt;&lt;br /&gt;
When looking at the internuclear distances vs time graph, when you swap r1 and r2 around, the graph follows the same trend except the lines for r1 and r2 change around. This is because now r1 decreases distance slightly as it becomes the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule with time and r2 increases distance with time as the H atom moves away. After about 15 seconds, the reaction has finished as r1 is just oscillating around the H-H bond distance and the other H atom has moved away fully. This is shown by figure 5 and 6. Again for the momenta vs time graph, when you change r1 and r2, the two lines in the graph follow the same trend but they are now swapped over. This is because now p2 increases over time and so the momentum of this H atom moving away increases faster and then plateaus once it has moved fully away and has no attraction to the molecule. For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule the momenta oscillates. This is shown by figure 7 and 8.&lt;br /&gt;
[[file:internuclear1pt1118.png|thumb|200px|Figure 5- Internuclear distance vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:internuclear2pt1118.png|thumb|200px|Figure 6- Internuclear distance vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta1pt1118.png|thumb|200px|Figure 7- Momenta vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta2pt1118.png|thumb|200px|Figure 8- Momenta vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed.&lt;br /&gt;
What do you observe?&amp;lt;/b&amp;gt;&lt;br /&gt;
To get the final positions the &#039;get last geometry&#039; function was used. The final r1=74.04pm, r2=352.59pm, p1=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2=-5.08g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Figures 9 and 10, show the internuclear distance vs time graph and the momenta vs time graph respectively. For the internuclear distance vs time graph the r1 distance increased to a maximum and the r2 distance decreased to a minimum over time. They increased and decreased to the distance at which the transition state is achieved so r1=r2=rts. For the momenta vs time graph, the p2 increased as the H atom approached the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and then reached zero when the transition state was reached again. It continued to increase again as the r2 distance increased again. p1 also increased but in an oscillating fashion, it plateaued when momenta was zero for a bit, when in the transition state, and then over time increased again after the transition state had passed.&lt;br /&gt;
[[file:finalinternuclearpt1118.png|thumb|200px|Figure 9- This is the internuclear distance vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
[[file:finalmomentapt1118.png|thumb|200px|Figure 10- This is the momenta vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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====Question 4: Complete the table by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
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A is the approach H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! p1/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  p2/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 ||-414.280 ||Reactive||The black line shows the reaction dynamics, the AB distance decreases as A approaches BC. The BC distance increases, until the transition state is reached. The reaction occurs and so the transition state is past and AB molecule is formed as C moves away. The black line passes down the product energy valley. ||[[file:row1_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.077 ||no reaction||The black line shows that the AB distance decreases to get to the transition state however, the transition state can not be reached. This is because there&#039;s not enough kinetic energy to get to the transition state and so overcome the energy barrier and form the products and it goes back to the reactants. The black line curves round as A starts to move away from molecule BC again. ||[[file:row2_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1|| -413.977 ||reactive||This reaction dynamic is very similar to the first one. A approaches BC, the AB distance decreases and the BC distance slightly increases therefore, forming the transition state. There&#039;s enough kinetic energy and so the reaction occurs. AB molecule forms and the black line shows this as it travels down the valley of the product energy. ||[[file:row3_pt1118.png|200px]]&lt;br /&gt;
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| -5.1 || -10.1|| -357.277 ||no reaction  ||From looking at the black line it can be seen that A approaches BC and some interaction forms, the transition state is reached. C still has some attraction to B . B moves between A and C, but goes back to form a molecule with C. The p2 is not large enough for the reaction to continue to form the products. There is enough kinetic energy for the reaction to occur, however, not all this kinetic energy may be as translational energy which is important for the reaction to occur. It is instead vibrational energy of the BC molecule.||[[file:row4_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 ||-349.477 ||reactive ||It can be seen that A moves towards BC and BC distance becomes larger, eventually getting to the transition state. B moves back and forth between A and C forming molecules with both. Eventually, B gets closer to A and further from C and so forming AB molecule, this time p2 is large enough and so the reaction can occur. ||[[file:row5_pt1118.png|200px]] &lt;br /&gt;
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To conclude, in order for a reaction to occur there needs to be enough kinetic energy. Enough of this kinetic energy needs to be translational energy, if all the kinetic energy is vibrational energy of the reactants molecule then the reaction won&#039;t occur. Reaction 1 and 3 show that when p1 is higher the reaction will occur faster. Lastly, p1 and p2 need to both be large enough in order for them to collide and for a reaction to occur as shown by the 4th and 5th set of conditions.&lt;br /&gt;
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{{fontcolor1|green|Good descriptions in the table. Be careful with the descriptions with A / B / C etc as this can get a bit confusing. You have concluded the work well here. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:09, 4 June 2020 (BST)}}&lt;br /&gt;
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====Question 5: Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
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Transition state theory assumes that if the reactants have enough energy the transition state will be reached and it will go on to form the products. However, even if there&#039;s enough kinetic energy, then it doesn&#039;t always mean a reaction will occur. This is shown by experimental values. The energy has to be spread correctly, for example as translational energy and not just vibrational energy of the molecule. Therefore, this will decrease the experimental rate because not all the kinetic energy is used as translational energy for the reaction.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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Transition state theory also assumes that once you go past the transition state and on to form the products that you cannot go back to form the reactants again. However, in experiment this is possible. Experiment 4 in the table above is an example of this, the reaction doesn&#039;t occur even though the transition state is reached. This also means the experimental rate is lower than predicted as not all the reactants will turn into products even if the transition state is reached.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; &lt;br /&gt;
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{{fontcolor1|green| Good well answered. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:13, 4 June 2020 (BST)}}&lt;br /&gt;
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It also assumes that the reaction can be treated classically, but quantum effects do occur in experiment. For example quantum tunnelling, this increases the experimental rate compared to the prediction. &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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The transition state theory lastly assumes a quasi-equilibrium between the reactants and transition state.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; How much transition state you get is determined by how much reactant you have and so this determines how much product you will get. However, in experiment there may not be an equilibrium, and therefore, this would mean the experimental rate value would be higher than predicted.&lt;br /&gt;
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{{fontcolor1|green|The experiment in this case is representative of one particular momenta combination of atom and molecule. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:13, 4 June 2020 (BST)}}&lt;br /&gt;
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===&amp;lt;u&amp;gt;Exercise 2&amp;lt;/u&amp;gt;===&lt;br /&gt;
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====Question 1/2: By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? Locate the approximate position of the transition state.====&lt;br /&gt;
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A= F, B=H, C=H&lt;br /&gt;
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F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. This reaction is exothermic, the energy of the reactants are higher than that of the products. This is an exothermic reaction because it forms stronger bonds in the products than those which are in the reactants,  it forms HF which has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. More energy is released when the HF bond forms than is needed to break the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond. This also means the transition state will be more similar to the reactants, it is an early transition state. Therefore, the transition state is near to when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the reactant and the minimum pathway on the left (AB) is the product. Therefore, you can see the product energy is lower than the reactant energy and so it&#039;s exothermic.&lt;br /&gt;
The enthalpy change for this reaction is -129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
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{{fontcolor1|green| Good referencing the figure here.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:24, 4 June 2020 (BST)}}&lt;br /&gt;
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HF+H. This reaction is endothermic, the energy of the reactants are lower than that of the products. HF has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, therefore, energy needs to be put into the reaction to break this bond and so the reaction is endothermic. More energy is needed to break the HF bond than is released when the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond is formed. This means that the transition state will be more similar to the products, it is a late transition state. Therefore, the transition state is near when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the product and the minimum pathway on the left is the reactant. Therefore, you can see the reactant energy is higher than the product energy and so it&#039;s endothermic.&lt;br /&gt;
The enthalpy change for this reaction is 129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
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Both reactions have the same transition state as they are the same reactions just going in opposite directions. I found the transition by finding where the force equals zero and then checking using the internuclear distances vs time graph to see that the graph was zero. This can be seen in figure 11.&lt;br /&gt;
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{{fontcolor1|green|Make sure to name figures numerically as they are referenced in the text, here 11 follows from 12. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:24, 4 June 2020 (BST)}}&lt;br /&gt;
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&lt;br /&gt;
[[file:HHFtspt1118.png|thumb|left|200px|Figure 11- Shows the internuclear distance vs time graph of the transition state of the HF + H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reactions]]&lt;br /&gt;
[[File:Screen Shot 2020-05-22 at 11.14.01.png|thumb|200px|Figure 12- This shows the surface plot for the reactions of H+HF and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F. AB distance is showing F approaching H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and BC distance is showing H approaching HF. AB is the distance between F and H and BC is the distance between H and H.]]&lt;br /&gt;
&lt;br /&gt;
====Question 3: Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy can be determined by taking away the energy of the reactants from the transition state energy.&lt;br /&gt;
&lt;br /&gt;
Using LEPS GUI and changing the distances of AB and BC, the energies for the H-F and H-H bonds can be determined. For the H-F bond energy I found to be -560.404 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is similar to -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; which it says in literature. To find this energy, I set the AB distance as 91pm and the BC distance as 4000pm so that the H atom (C) is so far away it doesn&#039;t give any interaction on the HF bond. For the H-H bond energy I found it to be -435.057 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, again this is close to the literature which was -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. To find this energy, I set the AB distance as 4000pm and the BC distance as 74.5pm. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good description and compariing to literature.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:24, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--435.057=1.076 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy of HF + H= -433.981--560.404=126.423 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy can also be determined using an MEP calculation and slightly displacing the transition state towards the reactants, this is a more accurate method because in the above method we are assuming that moving the atoms far apart will give us pure reactants.&lt;br /&gt;
&lt;br /&gt;
To determine activation energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the AB distance=182 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a very small drop in the graph and so using the initial and final energies the activation energy can be determined. Figure 13 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--434.144=0.163 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAEpt1118.png|thumb|200px|Figure 13- this shows the energy vs time graph used to calculate the activation energy for the reaction of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
&lt;br /&gt;
To determine activation energy of HF+H, the AB distance=180 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a drop in the graph and so using the two horizontal lines the activation energy can be determined. Figure 14 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of HF + H= -433.981--560.063= 126.082 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAE2pt1118.png|thumb|200px|Figure 14- this shows the energy vs time graph used to calculate the activation energy for the reaction of HF+F.]]&lt;br /&gt;
&lt;br /&gt;
Overall both methods give very similar values for the activation energies of the reactions.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Very well done, great answer and good comparison. You have made it really clear how you determined the energies in both cases and the calculations are sound. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:24, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====Question 4: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;br /&gt;
&lt;br /&gt;
Reaction conditions for a reactive trajectory of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F are rHF= AB distance =180 pm, rHH= BC distance = 74 pm, pHF=AB momentum= -1.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and pHH= BC momentum= 0.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The number of steps is 3000. &lt;br /&gt;
&lt;br /&gt;
The energy is conserved, therefore, the potential energy is converted to kinetic energy. This can be seen by the increase in oscillation in figure 15, once the transition state has been overcome and products starting to form. A large amount of the total energy goes to being vibrational energy of the product.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; The product molecule is oscillating lots therefore, can see that this is vibrational energy. Translational energy directs it to get over the potential energy barrier and then it can drop down and the energy becomes vibrational kinetic energy.&lt;br /&gt;
&lt;br /&gt;
[[File:Reactiondynamicspt1118.png|thumb|200px|Figure 15- This is contour plot showing the reaction dynamics of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is BC and F is A.]]&lt;br /&gt;
&lt;br /&gt;
It can be confirmed experimentally as the reactants and products have different vibrational energy states, and so can be tested using IR spectroscopy. It can be checked by looking either at the emission or absorption of the molecules. &lt;br /&gt;
For the reactants all the molecules are in the ground state, when it forms the products some of the molecules are excited, therefore, the some of the products are in the ground state and some in the first excited state. &lt;br /&gt;
When looking at absorption, you can see for the reactants the molecules in the ground state will get excited to the first excited energy level. Therefore, there is only one transition and so there will be only one peak in the IR spectrum. For the products, two transitions can occur, the molecules in the ground state can be excited to the first excited energy level (fundamental transition), and the molecules that are already in the first excited state will be excited to the second excited state (this is an overtone). These two transitions absorb at two different wavelengths. The IR spectrum will now have the same peak as the reactants as well as a peak at a lower wavenumber. This second peak is at a lower wavenumber because the difference between the first and second state is smaller than the difference between the ground state and first excited state, this is due to the anharmonicity of the system. Overtime the intensity of this overtone will decrease and the intensity of the fundamental will increase as molecules fall back down to the ground state. For looking at emission, instead of the molecules being excited they will fall back to the ground state and so light is emitted. This time, the reactant IR will have no peaks as all molecules are already in the ground state. For the products, there will be one peak as the molecules in the first excited state drop back down to the ground state. &lt;br /&gt;
&lt;br /&gt;
Chemiluminescence experiments can be run to study these reactions.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Setup a calculation starting on the side of the reactants of F + H2, at the bottom of the well rHH = 74 pm, with a momentum pFH = -1.0 g.mol-1.pm.fs-1, and explore several values of pHH in the range -6.1 to 6.1 g.mol-1.pm.fs-1 (explore values also close to these limits). What do you observe? &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The initial  rHF distance= 230 pm. A=F B=H C=H&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! pHF/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  pHH/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -6.0 ||-404.014 ||reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule oscillates as it approaches the F atom. At a time when the H atoms in the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule are repelling one another, there is an interaction between the F atom and the H atom (B). The H atom (B) bounces to and fro between the H (C) and F atoms, eventually forms a HF molecule when the other H atom starts to move away. The products oscillate more than the reactants, therefore, they have more vibrational energy.||[[file:row11_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -4.5 || -418.264 ||no reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule moves towards the F atom. The H atom (B) moves towards the F atom and forms the transition state but this atom then bounces back forming H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and moving away. Therefore, the energy barrier is not quite overcome as it rolls back to the reactants.||[[file:row22_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -2.0|| -432.014 ||no reaction||The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule starts to approach the F atom but there is not enough kinetic energy which is vibrational and in the correct direction for the transition state to be reached. The potential energy barrier can not be over come and so it rolls back to the reactants and no reaction occurs.||[[file:row33_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 2.0|| -428.014||no reaction ||This has the same trajectory as above except the molecules have a bit more vibrational energy as it oscillates a bit more. Again there&#039;s still not enough vibrational kinetic energy for the reactants to get over the potential energy barrier and a reaction to occur.||[[file:row44_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 6.0 ||-349.477 ||no reaction || The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; moves towards the F atom and the transition state is achieved. However, no reaction occurs and the molecules roll back to the reactants as opposed to the products. When the transition state is reached the H atom (B) bounces straight back to form the reactants again.||[[file:row55_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;For the same initial position, increase slightly the momentum pFH = -1.6 g.mol-1.pm.fs-1, and considerably reduce the overall energy of the system by reducing the momentum pHH = 0.2 g.mol-1.pm.fs-1. What do you observe now?&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[file:figure16pt1118.png|thumb|200px|Figure 16- This shows the trajectory for the reaction that occurs between H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and F atom, when pBC= pHH = 0.2 g.mol-1.pm.fs-1 and pAB= pFH = -1.6 g.mol-1.pm.fs-1. BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and A is the F atom. ]]&lt;br /&gt;
&lt;br /&gt;
The reaction occurs. The vibrational energy of the products is much greater than that of the reactants, this can be seen in figure 16. This can be seen because the molecules in the product well oscillate more than the molecules in the reactant well. A lot of the potential energy has been converted to vibrational energy. The kinetic energy for this reaction is very low but, the amount of this that is vibrational is enough and in the correct direction in order for the reaction to occur. In this reaction the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F, the transition state is reached. H atom. (B) bounces between the F atom and H atom (C), eventually the H atom (C) moves away and the HF molecule forms.&lt;br /&gt;
&lt;br /&gt;
====Question 5: Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ====&lt;br /&gt;
&lt;br /&gt;
Polyani&#039;s rule is that vibrational energy is able to promote an endothermic reaction more efficiently than translational energy. This is because in an endothermic reaction it is a late transition state and so if translational energy is used to promote the reaction, then it will hit the potential energy barrier and bounce back, the products are higher in energy and so it can not be used to direct to them. Energy needs to be put in to get over the energy barrier. Using translational energy means the incoming atom will hit the molecule and just bounce back, it can&#039;t get over the energy barrier. This energy is not in the correct direction for a reaction to occur. If vibrational energy is used then the molecule will be oscillating in the correct direction for a reaction to take place and can pass over the energy barrier. Therefore, the vibrational energy is more efficient at promoting an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
In an exothermic reaction, translational energy is more efficient than vibrational energy, it has an early transition state. This is because the energy is going down hill. The molecule can now move along the potential energy surface and once it gets to the transition state it can be guided around and move along in the correct direction to form the products. The translational energy directs the reactants to the products. In an exothermic reaction, the transition state is early and so the activation energy is much lower and so easier to get over the potential energy barrier, no energy needs to be put into the system. Therefore, it can just roll down using translational energy and so translational energy is more efficient for this reaction over vibrational energy. For an exothermic reaction, the energy is mainly changed from the translational energy to the vibrational energy of the products.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== References==&lt;br /&gt;
1. K. J. Laidler. Chemical Kinetics. 3rd edition. Harper Collins. 1987&lt;br /&gt;
&lt;br /&gt;
2. Ch301.cm.utexas.edu. 2020. Bond Enthalpies. [online] Available at: &amp;lt;https://ch301.cm.utexas.edu/section2.php?target=thermo/thermochemistry/enthalpy-bonds.html&amp;gt; [Accessed 21 May 2020].&lt;br /&gt;
&lt;br /&gt;
3. Chemistry LibreTexts. 2020. Bond Energies. [online] Available at:&amp;lt;https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Supplemental_Modules_(Physical_and_Theoretical_Chemistry)/Chemical_Bonding/Fundamentals_of_Chemical_Bonding/Bond_Energies&amp;gt; [Accessed 21 May 2020].&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812766</id>
		<title>MRD:01547559</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812766"/>
		<updated>2020-06-04T18:13:28Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 5: Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Molecular Reaction Dynamics: Applications to triatomic systems- Poppy Tobolski==&lt;br /&gt;
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===&amp;lt;u&amp;gt;Exercise 1&amp;lt;/u&amp;gt;===&lt;br /&gt;
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NOTE- r1= BC distance, r2= AB distance, p1= BC momentum, p2= AB momentum. However, it doesn&#039;t matter because this is a symmetrical system.&lt;br /&gt;
&lt;br /&gt;
==== Question 1: On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state resembles that of the reactants or products depending on which it is closer in energy to. In an exothermic reaction, the transition state is closer in energy to the reactants therefore, it resembles that of the reactants over the products. This is an early transition state. In an endothermic reaction the transition state is closer in energy to the products and so the transition state resembles that of the products. This is a late transition state. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|TGood introduction - a reference for Hammonds postulate may help here [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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The transition state is mathematically defined as ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0,  it&#039;s the point where the gradient equals zero. The transition state is at the local maximum within the well of minima, the saddle point. In the surface plot, there is a minimum path that connects the products to the reactants. The transition state can be identified as it is the maxima in this path, this is shown in figure 1. &lt;br /&gt;
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{{fontcolor1|green|Ok, the saddle is where the first partial derivative = 0 in both the reaction and orthogonal to the reaction co-ordinates. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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At the transition state, the H atoms do not move because force is a derivative of the potential energy. Therefore, force is zero and so the atoms are stationary.&lt;br /&gt;
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[[file:transitionstatemaximum_pt1118.png|300px|thumb|Figure 1-This graph is the surface plot for the reaction of H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. In this image, you can see there is a maximum is the minimum energy path, this shows the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
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{{fontcolor1|green|A second derivative will allow you to determine which direction the maxima and minima are in. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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==== Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
rAB= rBC=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.77pm&lt;br /&gt;
&lt;br /&gt;
When the distance between each of the H atoms equals this the force along the distances is very close to zero. Force is a derivative of the potential energy, and so when it equals zero it means the nuclei in the transition state are zero. It can be seen in figure 2 that the internuclear distance isn&#039;t changing with time when at the transition state, this is because the atoms are stationary.&lt;br /&gt;
&lt;br /&gt;
[[file:forceequalszeropt1118.png|300px|thumb|left|Figure 2-This graph is of the internuclear distance vs time for the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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{{fontcolor1|green|Well described. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:02, 4 June 2020 (BST)}}&lt;br /&gt;
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==== Question 3: Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
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When the MEP calculation is used the path is straight, however, when the dynamic calculation is used the path becomes curved. This is because the molecule is oscillating, but in the MEP calculation this is being ignored. The velocity is zero in the MEP calculation, so the path follows the minima on the valley floor of the product. The MEP calculation is not as realistic as the dynamic calculation, this is because it doesn&#039;t take into account that the atoms have masses and in MEP calculation the molecules have uniform motion. Figures 3 and 4 show this on a contour plot.&lt;br /&gt;
[[file:dynamicpt1118.png|thumb|200px|Figure 3- Contour plot of r1=rts+1 vs r2=rts, dynamic calculation has been used. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:meppt1118.png|thumb|200px|Figure 4- Contour plot of r1=rts+1 vs r2=rts, MEP calculation has been used. A is the approaching H atom and BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
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{{fontcolor1|green|I tihnk a little more information is required here on  the differences between MEP and dynamics. Good description regardless. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:04, 4 June 2020 (BST)}}&lt;br /&gt;
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&amp;lt;b&amp;gt;Look at the “Internuclear Distances vs Time” and “Momenta vs Time”. What would change if we used the initial conditions r1 = rts and r2 = rts+1 pm instead?&amp;lt;/b&amp;gt;&lt;br /&gt;
When looking at the internuclear distances vs time graph, when you swap r1 and r2 around, the graph follows the same trend except the lines for r1 and r2 change around. This is because now r1 decreases distance slightly as it becomes the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule with time and r2 increases distance with time as the H atom moves away. After about 15 seconds, the reaction has finished as r1 is just oscillating around the H-H bond distance and the other H atom has moved away fully. This is shown by figure 5 and 6. Again for the momenta vs time graph, when you change r1 and r2, the two lines in the graph follow the same trend but they are now swapped over. This is because now p2 increases over time and so the momentum of this H atom moving away increases faster and then plateaus once it has moved fully away and has no attraction to the molecule. For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule the momenta oscillates. This is shown by figure 7 and 8.&lt;br /&gt;
[[file:internuclear1pt1118.png|thumb|200px|Figure 5- Internuclear distance vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:internuclear2pt1118.png|thumb|200px|Figure 6- Internuclear distance vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta1pt1118.png|thumb|200px|Figure 7- Momenta vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta2pt1118.png|thumb|200px|Figure 8- Momenta vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed.&lt;br /&gt;
What do you observe?&amp;lt;/b&amp;gt;&lt;br /&gt;
To get the final positions the &#039;get last geometry&#039; function was used. The final r1=74.04pm, r2=352.59pm, p1=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2=-5.08g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Figures 9 and 10, show the internuclear distance vs time graph and the momenta vs time graph respectively. For the internuclear distance vs time graph the r1 distance increased to a maximum and the r2 distance decreased to a minimum over time. They increased and decreased to the distance at which the transition state is achieved so r1=r2=rts. For the momenta vs time graph, the p2 increased as the H atom approached the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and then reached zero when the transition state was reached again. It continued to increase again as the r2 distance increased again. p1 also increased but in an oscillating fashion, it plateaued when momenta was zero for a bit, when in the transition state, and then over time increased again after the transition state had passed.&lt;br /&gt;
[[file:finalinternuclearpt1118.png|thumb|200px|Figure 9- This is the internuclear distance vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
[[file:finalmomentapt1118.png|thumb|200px|Figure 10- This is the momenta vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
&lt;br /&gt;
====Question 4: Complete the table by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
&lt;br /&gt;
A is the approach H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! p1/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  p2/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 ||-414.280 ||Reactive||The black line shows the reaction dynamics, the AB distance decreases as A approaches BC. The BC distance increases, until the transition state is reached. The reaction occurs and so the transition state is past and AB molecule is formed as C moves away. The black line passes down the product energy valley. ||[[file:row1_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.077 ||no reaction||The black line shows that the AB distance decreases to get to the transition state however, the transition state can not be reached. This is because there&#039;s not enough kinetic energy to get to the transition state and so overcome the energy barrier and form the products and it goes back to the reactants. The black line curves round as A starts to move away from molecule BC again. ||[[file:row2_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1|| -413.977 ||reactive||This reaction dynamic is very similar to the first one. A approaches BC, the AB distance decreases and the BC distance slightly increases therefore, forming the transition state. There&#039;s enough kinetic energy and so the reaction occurs. AB molecule forms and the black line shows this as it travels down the valley of the product energy. ||[[file:row3_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1|| -357.277 ||no reaction  ||From looking at the black line it can be seen that A approaches BC and some interaction forms, the transition state is reached. C still has some attraction to B . B moves between A and C, but goes back to form a molecule with C. The p2 is not large enough for the reaction to continue to form the products. There is enough kinetic energy for the reaction to occur, however, not all this kinetic energy may be as translational energy which is important for the reaction to occur. It is instead vibrational energy of the BC molecule.||[[file:row4_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 ||-349.477 ||reactive ||It can be seen that A moves towards BC and BC distance becomes larger, eventually getting to the transition state. B moves back and forth between A and C forming molecules with both. Eventually, B gets closer to A and further from C and so forming AB molecule, this time p2 is large enough and so the reaction can occur. ||[[file:row5_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
To conclude, in order for a reaction to occur there needs to be enough kinetic energy. Enough of this kinetic energy needs to be translational energy, if all the kinetic energy is vibrational energy of the reactants molecule then the reaction won&#039;t occur. Reaction 1 and 3 show that when p1 is higher the reaction will occur faster. Lastly, p1 and p2 need to both be large enough in order for them to collide and for a reaction to occur as shown by the 4th and 5th set of conditions.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good descriptions in the table. Be careful with the descriptions with A / B / C etc as this can get a bit confusing. You have concluded the work well here. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:09, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Question 5: Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
&lt;br /&gt;
Transition state theory assumes that if the reactants have enough energy the transition state will be reached and it will go on to form the products. However, even if there&#039;s enough kinetic energy, then it doesn&#039;t always mean a reaction will occur. This is shown by experimental values. The energy has to be spread correctly, for example as translational energy and not just vibrational energy of the molecule. Therefore, this will decrease the experimental rate because not all the kinetic energy is used as translational energy for the reaction.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Transition state theory also assumes that once you go past the transition state and on to form the products that you cannot go back to form the reactants again. However, in experiment this is possible. Experiment 4 in the table above is an example of this, the reaction doesn&#039;t occur even though the transition state is reached. This also means the experimental rate is lower than predicted as not all the reactants will turn into products even if the transition state is reached.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good well answered. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
It also assumes that the reaction can be treated classically, but quantum effects do occur in experiment. For example quantum tunnelling, this increases the experimental rate compared to the prediction. &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state theory lastly assumes a quasi-equilibrium between the reactants and transition state.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; How much transition state you get is determined by how much reactant you have and so this determines how much product you will get. However, in experiment there may not be an equilibrium, and therefore, this would mean the experimental rate value would be higher than predicted.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|The experiment in this case is representative of one particular momenta combination of atom and molecule. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===&amp;lt;u&amp;gt;Exercise 2&amp;lt;/u&amp;gt;===&lt;br /&gt;
 &lt;br /&gt;
====Question 1/2: By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
A= F, B=H, C=H&lt;br /&gt;
&lt;br /&gt;
F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. This reaction is exothermic, the energy of the reactants are higher than that of the products. This is an exothermic reaction because it forms stronger bonds in the products than those which are in the reactants,  it forms HF which has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. More energy is released when the HF bond forms than is needed to break the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond. This also means the transition state will be more similar to the reactants, it is an early transition state. Therefore, the transition state is near to when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the reactant and the minimum pathway on the left (AB) is the product. Therefore, you can see the product energy is lower than the reactant energy and so it&#039;s exothermic.&lt;br /&gt;
The enthalpy change for this reaction is -129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
&lt;br /&gt;
HF+H. This reaction is endothermic, the energy of the reactants are lower than that of the products. HF has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, therefore, energy needs to be put into the reaction to break this bond and so the reaction is endothermic. More energy is needed to break the HF bond than is released when the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond is formed. This means that the transition state will be more similar to the products, it is a late transition state. Therefore, the transition state is near when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the product and the minimum pathway on the left is the reactant. Therefore, you can see the reactant energy is higher than the product energy and so it&#039;s endothermic.&lt;br /&gt;
The enthalpy change for this reaction is 129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
&lt;br /&gt;
Both reactions have the same transition state as they are the same reactions just going in opposite directions. I found the transition by finding where the force equals zero and then checking using the internuclear distances vs time graph to see that the graph was zero. This can be seen in figure 11.&lt;br /&gt;
&lt;br /&gt;
[[file:HHFtspt1118.png|thumb|left|200px|Figure 11- Shows the internuclear distance vs time graph of the transition state of the HF + H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reactions]]&lt;br /&gt;
[[File:Screen Shot 2020-05-22 at 11.14.01.png|thumb|200px|Figure 12- This shows the surface plot for the reactions of H+HF and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F. AB distance is showing F approaching H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and BC distance is showing H approaching HF. AB is the distance between F and H and BC is the distance between H and H.]]&lt;br /&gt;
&lt;br /&gt;
====Question 3: Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy can be determined by taking away the energy of the reactants from the transition state energy.&lt;br /&gt;
&lt;br /&gt;
Using LEPS GUI and changing the distances of AB and BC, the energies for the H-F and H-H bonds can be determined. For the H-F bond energy I found to be -560.404 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is similar to -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; which it says in literature. To find this energy, I set the AB distance as 91pm and the BC distance as 4000pm so that the H atom (C) is so far away it doesn&#039;t give any interaction on the HF bond. For the H-H bond energy I found it to be -435.057 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, again this is close to the literature which was -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. To find this energy, I set the AB distance as 4000pm and the BC distance as 74.5pm. &lt;br /&gt;
&lt;br /&gt;
Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--435.057=1.076 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy of HF + H= -433.981--560.404=126.423 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy can also be determined using an MEP calculation and slightly displacing the transition state towards the reactants, this is a more accurate method because in the above method we are assuming that moving the atoms far apart will give us pure reactants.&lt;br /&gt;
&lt;br /&gt;
To determine activation energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the AB distance=182 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a very small drop in the graph and so using the initial and final energies the activation energy can be determined. Figure 13 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--434.144=0.163 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAEpt1118.png|thumb|200px|Figure 13- this shows the energy vs time graph used to calculate the activation energy for the reaction of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
&lt;br /&gt;
To determine activation energy of HF+H, the AB distance=180 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a drop in the graph and so using the two horizontal lines the activation energy can be determined. Figure 14 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of HF + H= -433.981--560.063= 126.082 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAE2pt1118.png|thumb|200px|Figure 14- this shows the energy vs time graph used to calculate the activation energy for the reaction of HF+F.]]&lt;br /&gt;
&lt;br /&gt;
Overall both methods give very similar values for the activation energies of the reactions.&lt;br /&gt;
&lt;br /&gt;
====Question 4: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;br /&gt;
&lt;br /&gt;
Reaction conditions for a reactive trajectory of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F are rHF= AB distance =180 pm, rHH= BC distance = 74 pm, pHF=AB momentum= -1.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and pHH= BC momentum= 0.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The number of steps is 3000. &lt;br /&gt;
&lt;br /&gt;
The energy is conserved, therefore, the potential energy is converted to kinetic energy. This can be seen by the increase in oscillation in figure 15, once the transition state has been overcome and products starting to form. A large amount of the total energy goes to being vibrational energy of the product.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; The product molecule is oscillating lots therefore, can see that this is vibrational energy. Translational energy directs it to get over the potential energy barrier and then it can drop down and the energy becomes vibrational kinetic energy.&lt;br /&gt;
&lt;br /&gt;
[[File:Reactiondynamicspt1118.png|thumb|200px|Figure 15- This is contour plot showing the reaction dynamics of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is BC and F is A.]]&lt;br /&gt;
&lt;br /&gt;
It can be confirmed experimentally as the reactants and products have different vibrational energy states, and so can be tested using IR spectroscopy. It can be checked by looking either at the emission or absorption of the molecules. &lt;br /&gt;
For the reactants all the molecules are in the ground state, when it forms the products some of the molecules are excited, therefore, the some of the products are in the ground state and some in the first excited state. &lt;br /&gt;
When looking at absorption, you can see for the reactants the molecules in the ground state will get excited to the first excited energy level. Therefore, there is only one transition and so there will be only one peak in the IR spectrum. For the products, two transitions can occur, the molecules in the ground state can be excited to the first excited energy level (fundamental transition), and the molecules that are already in the first excited state will be excited to the second excited state (this is an overtone). These two transitions absorb at two different wavelengths. The IR spectrum will now have the same peak as the reactants as well as a peak at a lower wavenumber. This second peak is at a lower wavenumber because the difference between the first and second state is smaller than the difference between the ground state and first excited state, this is due to the anharmonicity of the system. Overtime the intensity of this overtone will decrease and the intensity of the fundamental will increase as molecules fall back down to the ground state. For looking at emission, instead of the molecules being excited they will fall back to the ground state and so light is emitted. This time, the reactant IR will have no peaks as all molecules are already in the ground state. For the products, there will be one peak as the molecules in the first excited state drop back down to the ground state. &lt;br /&gt;
&lt;br /&gt;
Chemiluminescence experiments can be run to study these reactions.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Setup a calculation starting on the side of the reactants of F + H2, at the bottom of the well rHH = 74 pm, with a momentum pFH = -1.0 g.mol-1.pm.fs-1, and explore several values of pHH in the range -6.1 to 6.1 g.mol-1.pm.fs-1 (explore values also close to these limits). What do you observe? &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The initial  rHF distance= 230 pm. A=F B=H C=H&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! pHF/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  pHH/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -6.0 ||-404.014 ||reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule oscillates as it approaches the F atom. At a time when the H atoms in the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule are repelling one another, there is an interaction between the F atom and the H atom (B). The H atom (B) bounces to and fro between the H (C) and F atoms, eventually forms a HF molecule when the other H atom starts to move away. The products oscillate more than the reactants, therefore, they have more vibrational energy.||[[file:row11_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -4.5 || -418.264 ||no reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule moves towards the F atom. The H atom (B) moves towards the F atom and forms the transition state but this atom then bounces back forming H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and moving away. Therefore, the energy barrier is not quite overcome as it rolls back to the reactants.||[[file:row22_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -2.0|| -432.014 ||no reaction||The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule starts to approach the F atom but there is not enough kinetic energy which is vibrational and in the correct direction for the transition state to be reached. The potential energy barrier can not be over come and so it rolls back to the reactants and no reaction occurs.||[[file:row33_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 2.0|| -428.014||no reaction ||This has the same trajectory as above except the molecules have a bit more vibrational energy as it oscillates a bit more. Again there&#039;s still not enough vibrational kinetic energy for the reactants to get over the potential energy barrier and a reaction to occur.||[[file:row44_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 6.0 ||-349.477 ||no reaction || The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; moves towards the F atom and the transition state is achieved. However, no reaction occurs and the molecules roll back to the reactants as opposed to the products. When the transition state is reached the H atom (B) bounces straight back to form the reactants again.||[[file:row55_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;For the same initial position, increase slightly the momentum pFH = -1.6 g.mol-1.pm.fs-1, and considerably reduce the overall energy of the system by reducing the momentum pHH = 0.2 g.mol-1.pm.fs-1. What do you observe now?&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[file:figure16pt1118.png|thumb|200px|Figure 16- This shows the trajectory for the reaction that occurs between H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and F atom, when pBC= pHH = 0.2 g.mol-1.pm.fs-1 and pAB= pFH = -1.6 g.mol-1.pm.fs-1. BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and A is the F atom. ]]&lt;br /&gt;
&lt;br /&gt;
The reaction occurs. The vibrational energy of the products is much greater than that of the reactants, this can be seen in figure 16. This can be seen because the molecules in the product well oscillate more than the molecules in the reactant well. A lot of the potential energy has been converted to vibrational energy. The kinetic energy for this reaction is very low but, the amount of this that is vibrational is enough and in the correct direction in order for the reaction to occur. In this reaction the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F, the transition state is reached. H atom. (B) bounces between the F atom and H atom (C), eventually the H atom (C) moves away and the HF molecule forms.&lt;br /&gt;
&lt;br /&gt;
====Question 5: Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ====&lt;br /&gt;
&lt;br /&gt;
Polyani&#039;s rule is that vibrational energy is able to promote an endothermic reaction more efficiently than translational energy. This is because in an endothermic reaction it is a late transition state and so if translational energy is used to promote the reaction, then it will hit the potential energy barrier and bounce back, the products are higher in energy and so it can not be used to direct to them. Energy needs to be put in to get over the energy barrier. Using translational energy means the incoming atom will hit the molecule and just bounce back, it can&#039;t get over the energy barrier. This energy is not in the correct direction for a reaction to occur. If vibrational energy is used then the molecule will be oscillating in the correct direction for a reaction to take place and can pass over the energy barrier. Therefore, the vibrational energy is more efficient at promoting an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
In an exothermic reaction, translational energy is more efficient than vibrational energy, it has an early transition state. This is because the energy is going down hill. The molecule can now move along the potential energy surface and once it gets to the transition state it can be guided around and move along in the correct direction to form the products. The translational energy directs the reactants to the products. In an exothermic reaction, the transition state is early and so the activation energy is much lower and so easier to get over the potential energy barrier, no energy needs to be put into the system. Therefore, it can just roll down using translational energy and so translational energy is more efficient for this reaction over vibrational energy. For an exothermic reaction, the energy is mainly changed from the translational energy to the vibrational energy of the products.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== References==&lt;br /&gt;
1. K. J. Laidler. Chemical Kinetics. 3rd edition. Harper Collins. 1987&lt;br /&gt;
&lt;br /&gt;
2. Ch301.cm.utexas.edu. 2020. Bond Enthalpies. [online] Available at: &amp;lt;https://ch301.cm.utexas.edu/section2.php?target=thermo/thermochemistry/enthalpy-bonds.html&amp;gt; [Accessed 21 May 2020].&lt;br /&gt;
&lt;br /&gt;
3. Chemistry LibreTexts. 2020. Bond Energies. [online] Available at:&amp;lt;https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Supplemental_Modules_(Physical_and_Theoretical_Chemistry)/Chemical_Bonding/Fundamentals_of_Chemical_Bonding/Bond_Energies&amp;gt; [Accessed 21 May 2020].&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812765</id>
		<title>MRD:01547559</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812765"/>
		<updated>2020-06-04T18:09:14Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 4: Complete the table by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Molecular Reaction Dynamics: Applications to triatomic systems- Poppy Tobolski==&lt;br /&gt;
&lt;br /&gt;
===&amp;lt;u&amp;gt;Exercise 1&amp;lt;/u&amp;gt;===&lt;br /&gt;
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NOTE- r1= BC distance, r2= AB distance, p1= BC momentum, p2= AB momentum. However, it doesn&#039;t matter because this is a symmetrical system.&lt;br /&gt;
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==== Question 1: On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state resembles that of the reactants or products depending on which it is closer in energy to. In an exothermic reaction, the transition state is closer in energy to the reactants therefore, it resembles that of the reactants over the products. This is an early transition state. In an endothermic reaction the transition state is closer in energy to the products and so the transition state resembles that of the products. This is a late transition state. &lt;br /&gt;
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{{fontcolor1|green|TGood introduction - a reference for Hammonds postulate may help here [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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The transition state is mathematically defined as ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0,  it&#039;s the point where the gradient equals zero. The transition state is at the local maximum within the well of minima, the saddle point. In the surface plot, there is a minimum path that connects the products to the reactants. The transition state can be identified as it is the maxima in this path, this is shown in figure 1. &lt;br /&gt;
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{{fontcolor1|green|Ok, the saddle is where the first partial derivative = 0 in both the reaction and orthogonal to the reaction co-ordinates. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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At the transition state, the H atoms do not move because force is a derivative of the potential energy. Therefore, force is zero and so the atoms are stationary.&lt;br /&gt;
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[[file:transitionstatemaximum_pt1118.png|300px|thumb|Figure 1-This graph is the surface plot for the reaction of H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. In this image, you can see there is a maximum is the minimum energy path, this shows the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
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{{fontcolor1|green|A second derivative will allow you to determine which direction the maxima and minima are in. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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==== Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
rAB= rBC=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.77pm&lt;br /&gt;
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When the distance between each of the H atoms equals this the force along the distances is very close to zero. Force is a derivative of the potential energy, and so when it equals zero it means the nuclei in the transition state are zero. It can be seen in figure 2 that the internuclear distance isn&#039;t changing with time when at the transition state, this is because the atoms are stationary.&lt;br /&gt;
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[[file:forceequalszeropt1118.png|300px|thumb|left|Figure 2-This graph is of the internuclear distance vs time for the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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{{fontcolor1|green|Well described. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:02, 4 June 2020 (BST)}}&lt;br /&gt;
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==== Question 3: Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
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When the MEP calculation is used the path is straight, however, when the dynamic calculation is used the path becomes curved. This is because the molecule is oscillating, but in the MEP calculation this is being ignored. The velocity is zero in the MEP calculation, so the path follows the minima on the valley floor of the product. The MEP calculation is not as realistic as the dynamic calculation, this is because it doesn&#039;t take into account that the atoms have masses and in MEP calculation the molecules have uniform motion. Figures 3 and 4 show this on a contour plot.&lt;br /&gt;
[[file:dynamicpt1118.png|thumb|200px|Figure 3- Contour plot of r1=rts+1 vs r2=rts, dynamic calculation has been used. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:meppt1118.png|thumb|200px|Figure 4- Contour plot of r1=rts+1 vs r2=rts, MEP calculation has been used. A is the approaching H atom and BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
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{{fontcolor1|green|I tihnk a little more information is required here on  the differences between MEP and dynamics. Good description regardless. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:04, 4 June 2020 (BST)}}&lt;br /&gt;
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&amp;lt;b&amp;gt;Look at the “Internuclear Distances vs Time” and “Momenta vs Time”. What would change if we used the initial conditions r1 = rts and r2 = rts+1 pm instead?&amp;lt;/b&amp;gt;&lt;br /&gt;
When looking at the internuclear distances vs time graph, when you swap r1 and r2 around, the graph follows the same trend except the lines for r1 and r2 change around. This is because now r1 decreases distance slightly as it becomes the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule with time and r2 increases distance with time as the H atom moves away. After about 15 seconds, the reaction has finished as r1 is just oscillating around the H-H bond distance and the other H atom has moved away fully. This is shown by figure 5 and 6. Again for the momenta vs time graph, when you change r1 and r2, the two lines in the graph follow the same trend but they are now swapped over. This is because now p2 increases over time and so the momentum of this H atom moving away increases faster and then plateaus once it has moved fully away and has no attraction to the molecule. For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule the momenta oscillates. This is shown by figure 7 and 8.&lt;br /&gt;
[[file:internuclear1pt1118.png|thumb|200px|Figure 5- Internuclear distance vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:internuclear2pt1118.png|thumb|200px|Figure 6- Internuclear distance vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta1pt1118.png|thumb|200px|Figure 7- Momenta vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta2pt1118.png|thumb|200px|Figure 8- Momenta vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed.&lt;br /&gt;
What do you observe?&amp;lt;/b&amp;gt;&lt;br /&gt;
To get the final positions the &#039;get last geometry&#039; function was used. The final r1=74.04pm, r2=352.59pm, p1=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2=-5.08g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Figures 9 and 10, show the internuclear distance vs time graph and the momenta vs time graph respectively. For the internuclear distance vs time graph the r1 distance increased to a maximum and the r2 distance decreased to a minimum over time. They increased and decreased to the distance at which the transition state is achieved so r1=r2=rts. For the momenta vs time graph, the p2 increased as the H atom approached the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and then reached zero when the transition state was reached again. It continued to increase again as the r2 distance increased again. p1 also increased but in an oscillating fashion, it plateaued when momenta was zero for a bit, when in the transition state, and then over time increased again after the transition state had passed.&lt;br /&gt;
[[file:finalinternuclearpt1118.png|thumb|200px|Figure 9- This is the internuclear distance vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
[[file:finalmomentapt1118.png|thumb|200px|Figure 10- This is the momenta vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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====Question 4: Complete the table by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
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A is the approach H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! p1/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  p2/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
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| -2.56 || -5.1 ||-414.280 ||Reactive||The black line shows the reaction dynamics, the AB distance decreases as A approaches BC. The BC distance increases, until the transition state is reached. The reaction occurs and so the transition state is past and AB molecule is formed as C moves away. The black line passes down the product energy valley. ||[[file:row1_pt1118.png|200px]]&lt;br /&gt;
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| -3.1 || -4.1 || -420.077 ||no reaction||The black line shows that the AB distance decreases to get to the transition state however, the transition state can not be reached. This is because there&#039;s not enough kinetic energy to get to the transition state and so overcome the energy barrier and form the products and it goes back to the reactants. The black line curves round as A starts to move away from molecule BC again. ||[[file:row2_pt1118.png|200px]]&lt;br /&gt;
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| -3.1 || -5.1|| -413.977 ||reactive||This reaction dynamic is very similar to the first one. A approaches BC, the AB distance decreases and the BC distance slightly increases therefore, forming the transition state. There&#039;s enough kinetic energy and so the reaction occurs. AB molecule forms and the black line shows this as it travels down the valley of the product energy. ||[[file:row3_pt1118.png|200px]]&lt;br /&gt;
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| -5.1 || -10.1|| -357.277 ||no reaction  ||From looking at the black line it can be seen that A approaches BC and some interaction forms, the transition state is reached. C still has some attraction to B . B moves between A and C, but goes back to form a molecule with C. The p2 is not large enough for the reaction to continue to form the products. There is enough kinetic energy for the reaction to occur, however, not all this kinetic energy may be as translational energy which is important for the reaction to occur. It is instead vibrational energy of the BC molecule.||[[file:row4_pt1118.png|200px]] &lt;br /&gt;
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| -5.1 || -10.6 ||-349.477 ||reactive ||It can be seen that A moves towards BC and BC distance becomes larger, eventually getting to the transition state. B moves back and forth between A and C forming molecules with both. Eventually, B gets closer to A and further from C and so forming AB molecule, this time p2 is large enough and so the reaction can occur. ||[[file:row5_pt1118.png|200px]] &lt;br /&gt;
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To conclude, in order for a reaction to occur there needs to be enough kinetic energy. Enough of this kinetic energy needs to be translational energy, if all the kinetic energy is vibrational energy of the reactants molecule then the reaction won&#039;t occur. Reaction 1 and 3 show that when p1 is higher the reaction will occur faster. Lastly, p1 and p2 need to both be large enough in order for them to collide and for a reaction to occur as shown by the 4th and 5th set of conditions.&lt;br /&gt;
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{{fontcolor1|green|Good descriptions in the table. Be careful with the descriptions with A / B / C etc as this can get a bit confusing. You have concluded the work well here. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:09, 4 June 2020 (BST)}}&lt;br /&gt;
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====Question 5: Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
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Transition state theory assumes that if the reactants have enough energy the transition state will be reached and it will go on to form the products. However, even if there&#039;s enough kinetic energy, then it doesn&#039;t always mean a reaction will occur. This is shown by experimental values. The energy has to be spread correctly, for example as translational energy and not just vibrational energy of the molecule. Therefore, this will decrease the experimental rate because not all the kinetic energy is used as translational energy for the reaction.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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Transition state theory also assumes that once you go past the transition state and on to form the products that you cannot go back to form the reactants again. However, in experiment this is possible. Experiment 4 in the table above is an example of this, the reaction doesn&#039;t occur even though the transition state is reached. This also means the experimental rate is lower than predicted as not all the reactants will turn into products even if the transition state is reached.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; &lt;br /&gt;
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It also assumes that the reaction can be treated classically, but quantum effects do occur in experiment. For example quantum tunnelling, this increases the experimental rate compared to the prediction. &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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The transition state theory lastly assumes a quasi-equilibrium between the reactants and transition state.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; How much transition state you get is determined by how much reactant you have and so this determines how much product you will get. However, in experiment there may not be an equilibrium, and therefore, this would mean the experimental rate value would be higher than predicted.&lt;br /&gt;
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===&amp;lt;u&amp;gt;Exercise 2&amp;lt;/u&amp;gt;===&lt;br /&gt;
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====Question 1/2: By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? Locate the approximate position of the transition state.====&lt;br /&gt;
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A= F, B=H, C=H&lt;br /&gt;
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F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. This reaction is exothermic, the energy of the reactants are higher than that of the products. This is an exothermic reaction because it forms stronger bonds in the products than those which are in the reactants,  it forms HF which has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. More energy is released when the HF bond forms than is needed to break the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond. This also means the transition state will be more similar to the reactants, it is an early transition state. Therefore, the transition state is near to when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the reactant and the minimum pathway on the left (AB) is the product. Therefore, you can see the product energy is lower than the reactant energy and so it&#039;s exothermic.&lt;br /&gt;
The enthalpy change for this reaction is -129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
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HF+H. This reaction is endothermic, the energy of the reactants are lower than that of the products. HF has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, therefore, energy needs to be put into the reaction to break this bond and so the reaction is endothermic. More energy is needed to break the HF bond than is released when the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond is formed. This means that the transition state will be more similar to the products, it is a late transition state. Therefore, the transition state is near when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the product and the minimum pathway on the left is the reactant. Therefore, you can see the reactant energy is higher than the product energy and so it&#039;s endothermic.&lt;br /&gt;
The enthalpy change for this reaction is 129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
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Both reactions have the same transition state as they are the same reactions just going in opposite directions. I found the transition by finding where the force equals zero and then checking using the internuclear distances vs time graph to see that the graph was zero. This can be seen in figure 11.&lt;br /&gt;
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[[file:HHFtspt1118.png|thumb|left|200px|Figure 11- Shows the internuclear distance vs time graph of the transition state of the HF + H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reactions]]&lt;br /&gt;
[[File:Screen Shot 2020-05-22 at 11.14.01.png|thumb|200px|Figure 12- This shows the surface plot for the reactions of H+HF and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F. AB distance is showing F approaching H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and BC distance is showing H approaching HF. AB is the distance between F and H and BC is the distance between H and H.]]&lt;br /&gt;
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====Question 3: Report the activation energy for both reactions.====&lt;br /&gt;
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The activation energy can be determined by taking away the energy of the reactants from the transition state energy.&lt;br /&gt;
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Using LEPS GUI and changing the distances of AB and BC, the energies for the H-F and H-H bonds can be determined. For the H-F bond energy I found to be -560.404 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is similar to -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; which it says in literature. To find this energy, I set the AB distance as 91pm and the BC distance as 4000pm so that the H atom (C) is so far away it doesn&#039;t give any interaction on the HF bond. For the H-H bond energy I found it to be -435.057 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, again this is close to the literature which was -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. To find this energy, I set the AB distance as 4000pm and the BC distance as 74.5pm. &lt;br /&gt;
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Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--435.057=1.076 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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Activation energy of HF + H= -433.981--560.404=126.423 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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The activation energy can also be determined using an MEP calculation and slightly displacing the transition state towards the reactants, this is a more accurate method because in the above method we are assuming that moving the atoms far apart will give us pure reactants.&lt;br /&gt;
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To determine activation energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the AB distance=182 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a very small drop in the graph and so using the initial and final energies the activation energy can be determined. Figure 13 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--434.144=0.163 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAEpt1118.png|thumb|200px|Figure 13- this shows the energy vs time graph used to calculate the activation energy for the reaction of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
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To determine activation energy of HF+H, the AB distance=180 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a drop in the graph and so using the two horizontal lines the activation energy can be determined. Figure 14 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of HF + H= -433.981--560.063= 126.082 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAE2pt1118.png|thumb|200px|Figure 14- this shows the energy vs time graph used to calculate the activation energy for the reaction of HF+F.]]&lt;br /&gt;
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Overall both methods give very similar values for the activation energies of the reactions.&lt;br /&gt;
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====Question 4: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;br /&gt;
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Reaction conditions for a reactive trajectory of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F are rHF= AB distance =180 pm, rHH= BC distance = 74 pm, pHF=AB momentum= -1.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and pHH= BC momentum= 0.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The number of steps is 3000. &lt;br /&gt;
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The energy is conserved, therefore, the potential energy is converted to kinetic energy. This can be seen by the increase in oscillation in figure 15, once the transition state has been overcome and products starting to form. A large amount of the total energy goes to being vibrational energy of the product.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; The product molecule is oscillating lots therefore, can see that this is vibrational energy. Translational energy directs it to get over the potential energy barrier and then it can drop down and the energy becomes vibrational kinetic energy.&lt;br /&gt;
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[[File:Reactiondynamicspt1118.png|thumb|200px|Figure 15- This is contour plot showing the reaction dynamics of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is BC and F is A.]]&lt;br /&gt;
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It can be confirmed experimentally as the reactants and products have different vibrational energy states, and so can be tested using IR spectroscopy. It can be checked by looking either at the emission or absorption of the molecules. &lt;br /&gt;
For the reactants all the molecules are in the ground state, when it forms the products some of the molecules are excited, therefore, the some of the products are in the ground state and some in the first excited state. &lt;br /&gt;
When looking at absorption, you can see for the reactants the molecules in the ground state will get excited to the first excited energy level. Therefore, there is only one transition and so there will be only one peak in the IR spectrum. For the products, two transitions can occur, the molecules in the ground state can be excited to the first excited energy level (fundamental transition), and the molecules that are already in the first excited state will be excited to the second excited state (this is an overtone). These two transitions absorb at two different wavelengths. The IR spectrum will now have the same peak as the reactants as well as a peak at a lower wavenumber. This second peak is at a lower wavenumber because the difference between the first and second state is smaller than the difference between the ground state and first excited state, this is due to the anharmonicity of the system. Overtime the intensity of this overtone will decrease and the intensity of the fundamental will increase as molecules fall back down to the ground state. For looking at emission, instead of the molecules being excited they will fall back to the ground state and so light is emitted. This time, the reactant IR will have no peaks as all molecules are already in the ground state. For the products, there will be one peak as the molecules in the first excited state drop back down to the ground state. &lt;br /&gt;
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Chemiluminescence experiments can be run to study these reactions.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Setup a calculation starting on the side of the reactants of F + H2, at the bottom of the well rHH = 74 pm, with a momentum pFH = -1.0 g.mol-1.pm.fs-1, and explore several values of pHH in the range -6.1 to 6.1 g.mol-1.pm.fs-1 (explore values also close to these limits). What do you observe? &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The initial  rHF distance= 230 pm. A=F B=H C=H&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! pHF/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  pHH/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -6.0 ||-404.014 ||reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule oscillates as it approaches the F atom. At a time when the H atoms in the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule are repelling one another, there is an interaction between the F atom and the H atom (B). The H atom (B) bounces to and fro between the H (C) and F atoms, eventually forms a HF molecule when the other H atom starts to move away. The products oscillate more than the reactants, therefore, they have more vibrational energy.||[[file:row11_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -4.5 || -418.264 ||no reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule moves towards the F atom. The H atom (B) moves towards the F atom and forms the transition state but this atom then bounces back forming H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and moving away. Therefore, the energy barrier is not quite overcome as it rolls back to the reactants.||[[file:row22_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -2.0|| -432.014 ||no reaction||The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule starts to approach the F atom but there is not enough kinetic energy which is vibrational and in the correct direction for the transition state to be reached. The potential energy barrier can not be over come and so it rolls back to the reactants and no reaction occurs.||[[file:row33_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 2.0|| -428.014||no reaction ||This has the same trajectory as above except the molecules have a bit more vibrational energy as it oscillates a bit more. Again there&#039;s still not enough vibrational kinetic energy for the reactants to get over the potential energy barrier and a reaction to occur.||[[file:row44_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 6.0 ||-349.477 ||no reaction || The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; moves towards the F atom and the transition state is achieved. However, no reaction occurs and the molecules roll back to the reactants as opposed to the products. When the transition state is reached the H atom (B) bounces straight back to form the reactants again.||[[file:row55_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;For the same initial position, increase slightly the momentum pFH = -1.6 g.mol-1.pm.fs-1, and considerably reduce the overall energy of the system by reducing the momentum pHH = 0.2 g.mol-1.pm.fs-1. What do you observe now?&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[file:figure16pt1118.png|thumb|200px|Figure 16- This shows the trajectory for the reaction that occurs between H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and F atom, when pBC= pHH = 0.2 g.mol-1.pm.fs-1 and pAB= pFH = -1.6 g.mol-1.pm.fs-1. BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and A is the F atom. ]]&lt;br /&gt;
&lt;br /&gt;
The reaction occurs. The vibrational energy of the products is much greater than that of the reactants, this can be seen in figure 16. This can be seen because the molecules in the product well oscillate more than the molecules in the reactant well. A lot of the potential energy has been converted to vibrational energy. The kinetic energy for this reaction is very low but, the amount of this that is vibrational is enough and in the correct direction in order for the reaction to occur. In this reaction the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F, the transition state is reached. H atom. (B) bounces between the F atom and H atom (C), eventually the H atom (C) moves away and the HF molecule forms.&lt;br /&gt;
&lt;br /&gt;
====Question 5: Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ====&lt;br /&gt;
&lt;br /&gt;
Polyani&#039;s rule is that vibrational energy is able to promote an endothermic reaction more efficiently than translational energy. This is because in an endothermic reaction it is a late transition state and so if translational energy is used to promote the reaction, then it will hit the potential energy barrier and bounce back, the products are higher in energy and so it can not be used to direct to them. Energy needs to be put in to get over the energy barrier. Using translational energy means the incoming atom will hit the molecule and just bounce back, it can&#039;t get over the energy barrier. This energy is not in the correct direction for a reaction to occur. If vibrational energy is used then the molecule will be oscillating in the correct direction for a reaction to take place and can pass over the energy barrier. Therefore, the vibrational energy is more efficient at promoting an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
In an exothermic reaction, translational energy is more efficient than vibrational energy, it has an early transition state. This is because the energy is going down hill. The molecule can now move along the potential energy surface and once it gets to the transition state it can be guided around and move along in the correct direction to form the products. The translational energy directs the reactants to the products. In an exothermic reaction, the transition state is early and so the activation energy is much lower and so easier to get over the potential energy barrier, no energy needs to be put into the system. Therefore, it can just roll down using translational energy and so translational energy is more efficient for this reaction over vibrational energy. For an exothermic reaction, the energy is mainly changed from the translational energy to the vibrational energy of the products.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== References==&lt;br /&gt;
1. K. J. Laidler. Chemical Kinetics. 3rd edition. Harper Collins. 1987&lt;br /&gt;
&lt;br /&gt;
2. Ch301.cm.utexas.edu. 2020. Bond Enthalpies. [online] Available at: &amp;lt;https://ch301.cm.utexas.edu/section2.php?target=thermo/thermochemistry/enthalpy-bonds.html&amp;gt; [Accessed 21 May 2020].&lt;br /&gt;
&lt;br /&gt;
3. Chemistry LibreTexts. 2020. Bond Energies. [online] Available at:&amp;lt;https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Supplemental_Modules_(Physical_and_Theoretical_Chemistry)/Chemical_Bonding/Fundamentals_of_Chemical_Bonding/Bond_Energies&amp;gt; [Accessed 21 May 2020].&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812764</id>
		<title>MRD:01547559</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812764"/>
		<updated>2020-06-04T18:04:28Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 3: Comment on how the mep and the trajectory you just calculated differ. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Molecular Reaction Dynamics: Applications to triatomic systems- Poppy Tobolski==&lt;br /&gt;
&lt;br /&gt;
===&amp;lt;u&amp;gt;Exercise 1&amp;lt;/u&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
NOTE- r1= BC distance, r2= AB distance, p1= BC momentum, p2= AB momentum. However, it doesn&#039;t matter because this is a symmetrical system.&lt;br /&gt;
&lt;br /&gt;
==== Question 1: On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state resembles that of the reactants or products depending on which it is closer in energy to. In an exothermic reaction, the transition state is closer in energy to the reactants therefore, it resembles that of the reactants over the products. This is an early transition state. In an endothermic reaction the transition state is closer in energy to the products and so the transition state resembles that of the products. This is a late transition state. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|TGood introduction - a reference for Hammonds postulate may help here [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0,  it&#039;s the point where the gradient equals zero. The transition state is at the local maximum within the well of minima, the saddle point. In the surface plot, there is a minimum path that connects the products to the reactants. The transition state can be identified as it is the maxima in this path, this is shown in figure 1. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, the saddle is where the first partial derivative = 0 in both the reaction and orthogonal to the reaction co-ordinates. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
At the transition state, the H atoms do not move because force is a derivative of the potential energy. Therefore, force is zero and so the atoms are stationary.&lt;br /&gt;
&lt;br /&gt;
[[file:transitionstatemaximum_pt1118.png|300px|thumb|Figure 1-This graph is the surface plot for the reaction of H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. In this image, you can see there is a maximum is the minimum energy path, this shows the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|A second derivative will allow you to determine which direction the maxima and minima are in. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
rAB= rBC=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.77pm&lt;br /&gt;
&lt;br /&gt;
When the distance between each of the H atoms equals this the force along the distances is very close to zero. Force is a derivative of the potential energy, and so when it equals zero it means the nuclei in the transition state are zero. It can be seen in figure 2 that the internuclear distance isn&#039;t changing with time when at the transition state, this is because the atoms are stationary.&lt;br /&gt;
&lt;br /&gt;
[[file:forceequalszeropt1118.png|300px|thumb|left|Figure 2-This graph is of the internuclear distance vs time for the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Well described. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Question 3: Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
&lt;br /&gt;
When the MEP calculation is used the path is straight, however, when the dynamic calculation is used the path becomes curved. This is because the molecule is oscillating, but in the MEP calculation this is being ignored. The velocity is zero in the MEP calculation, so the path follows the minima on the valley floor of the product. The MEP calculation is not as realistic as the dynamic calculation, this is because it doesn&#039;t take into account that the atoms have masses and in MEP calculation the molecules have uniform motion. Figures 3 and 4 show this on a contour plot.&lt;br /&gt;
[[file:dynamicpt1118.png|thumb|200px|Figure 3- Contour plot of r1=rts+1 vs r2=rts, dynamic calculation has been used. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:meppt1118.png|thumb|200px|Figure 4- Contour plot of r1=rts+1 vs r2=rts, MEP calculation has been used. A is the approaching H atom and BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|I tihnk a little more information is required here on  the differences between MEP and dynamics. Good description regardless. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Look at the “Internuclear Distances vs Time” and “Momenta vs Time”. What would change if we used the initial conditions r1 = rts and r2 = rts+1 pm instead?&amp;lt;/b&amp;gt;&lt;br /&gt;
When looking at the internuclear distances vs time graph, when you swap r1 and r2 around, the graph follows the same trend except the lines for r1 and r2 change around. This is because now r1 decreases distance slightly as it becomes the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule with time and r2 increases distance with time as the H atom moves away. After about 15 seconds, the reaction has finished as r1 is just oscillating around the H-H bond distance and the other H atom has moved away fully. This is shown by figure 5 and 6. Again for the momenta vs time graph, when you change r1 and r2, the two lines in the graph follow the same trend but they are now swapped over. This is because now p2 increases over time and so the momentum of this H atom moving away increases faster and then plateaus once it has moved fully away and has no attraction to the molecule. For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule the momenta oscillates. This is shown by figure 7 and 8.&lt;br /&gt;
[[file:internuclear1pt1118.png|thumb|200px|Figure 5- Internuclear distance vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:internuclear2pt1118.png|thumb|200px|Figure 6- Internuclear distance vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta1pt1118.png|thumb|200px|Figure 7- Momenta vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta2pt1118.png|thumb|200px|Figure 8- Momenta vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed.&lt;br /&gt;
What do you observe?&amp;lt;/b&amp;gt;&lt;br /&gt;
To get the final positions the &#039;get last geometry&#039; function was used. The final r1=74.04pm, r2=352.59pm, p1=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2=-5.08g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Figures 9 and 10, show the internuclear distance vs time graph and the momenta vs time graph respectively. For the internuclear distance vs time graph the r1 distance increased to a maximum and the r2 distance decreased to a minimum over time. They increased and decreased to the distance at which the transition state is achieved so r1=r2=rts. For the momenta vs time graph, the p2 increased as the H atom approached the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and then reached zero when the transition state was reached again. It continued to increase again as the r2 distance increased again. p1 also increased but in an oscillating fashion, it plateaued when momenta was zero for a bit, when in the transition state, and then over time increased again after the transition state had passed.&lt;br /&gt;
[[file:finalinternuclearpt1118.png|thumb|200px|Figure 9- This is the internuclear distance vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
[[file:finalmomentapt1118.png|thumb|200px|Figure 10- This is the momenta vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
&lt;br /&gt;
====Question 4: Complete the table by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
&lt;br /&gt;
A is the approach H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! p1/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  p2/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 ||-414.280 ||Reactive||The black line shows the reaction dynamics, the AB distance decreases as A approaches BC. The BC distance increases, until the transition state is reached. The reaction occurs and so the transition state is past and AB molecule is formed as C moves away. The black line passes down the product energy valley. ||[[file:row1_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.077 ||no reaction||The black line shows that the AB distance decreases to get to the transition state however, the transition state can not be reached. This is because there&#039;s not enough kinetic energy to get to the transition state and so overcome the energy barrier and form the products and it goes back to the reactants. The black line curves round as A starts to move away from molecule BC again. ||[[file:row2_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1|| -413.977 ||reactive||This reaction dynamic is very similar to the first one. A approaches BC, the AB distance decreases and the BC distance slightly increases therefore, forming the transition state. There&#039;s enough kinetic energy and so the reaction occurs. AB molecule forms and the black line shows this as it travels down the valley of the product energy. ||[[file:row3_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1|| -357.277 ||no reaction  ||From looking at the black line it can be seen that A approaches BC and some interaction forms, the transition state is reached. C still has some attraction to B . B moves between A and C, but goes back to form a molecule with C. The p2 is not large enough for the reaction to continue to form the products. There is enough kinetic energy for the reaction to occur, however, not all this kinetic energy may be as translational energy which is important for the reaction to occur. It is instead vibrational energy of the BC molecule.||[[file:row4_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 ||-349.477 ||reactive ||It can be seen that A moves towards BC and BC distance becomes larger, eventually getting to the transition state. B moves back and forth between A and C forming molecules with both. Eventually, B gets closer to A and further from C and so forming AB molecule, this time p2 is large enough and so the reaction can occur. ||[[file:row5_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
To conclude, in order for a reaction to occur there needs to be enough kinetic energy. Enough of this kinetic energy needs to be translational energy, if all the kinetic energy is vibrational energy of the reactants molecule then the reaction won&#039;t occur. Reaction 1 and 3 show that when p1 is higher the reaction will occur faster. Lastly, p1 and p2 need to both be large enough in order for them to collide and for a reaction to occur as shown by the 4th and 5th set of conditions.&lt;br /&gt;
&lt;br /&gt;
====Question 5: Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
&lt;br /&gt;
Transition state theory assumes that if the reactants have enough energy the transition state will be reached and it will go on to form the products. However, even if there&#039;s enough kinetic energy, then it doesn&#039;t always mean a reaction will occur. This is shown by experimental values. The energy has to be spread correctly, for example as translational energy and not just vibrational energy of the molecule. Therefore, this will decrease the experimental rate because not all the kinetic energy is used as translational energy for the reaction.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Transition state theory also assumes that once you go past the transition state and on to form the products that you cannot go back to form the reactants again. However, in experiment this is possible. Experiment 4 in the table above is an example of this, the reaction doesn&#039;t occur even though the transition state is reached. This also means the experimental rate is lower than predicted as not all the reactants will turn into products even if the transition state is reached.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; &lt;br /&gt;
&lt;br /&gt;
It also assumes that the reaction can be treated classically, but quantum effects do occur in experiment. For example quantum tunnelling, this increases the experimental rate compared to the prediction. &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state theory lastly assumes a quasi-equilibrium between the reactants and transition state.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; How much transition state you get is determined by how much reactant you have and so this determines how much product you will get. However, in experiment there may not be an equilibrium, and therefore, this would mean the experimental rate value would be higher than predicted.&lt;br /&gt;
&lt;br /&gt;
===&amp;lt;u&amp;gt;Exercise 2&amp;lt;/u&amp;gt;===&lt;br /&gt;
 &lt;br /&gt;
====Question 1/2: By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
A= F, B=H, C=H&lt;br /&gt;
&lt;br /&gt;
F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. This reaction is exothermic, the energy of the reactants are higher than that of the products. This is an exothermic reaction because it forms stronger bonds in the products than those which are in the reactants,  it forms HF which has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. More energy is released when the HF bond forms than is needed to break the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond. This also means the transition state will be more similar to the reactants, it is an early transition state. Therefore, the transition state is near to when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the reactant and the minimum pathway on the left (AB) is the product. Therefore, you can see the product energy is lower than the reactant energy and so it&#039;s exothermic.&lt;br /&gt;
The enthalpy change for this reaction is -129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
&lt;br /&gt;
HF+H. This reaction is endothermic, the energy of the reactants are lower than that of the products. HF has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, therefore, energy needs to be put into the reaction to break this bond and so the reaction is endothermic. More energy is needed to break the HF bond than is released when the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond is formed. This means that the transition state will be more similar to the products, it is a late transition state. Therefore, the transition state is near when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the product and the minimum pathway on the left is the reactant. Therefore, you can see the reactant energy is higher than the product energy and so it&#039;s endothermic.&lt;br /&gt;
The enthalpy change for this reaction is 129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
&lt;br /&gt;
Both reactions have the same transition state as they are the same reactions just going in opposite directions. I found the transition by finding where the force equals zero and then checking using the internuclear distances vs time graph to see that the graph was zero. This can be seen in figure 11.&lt;br /&gt;
&lt;br /&gt;
[[file:HHFtspt1118.png|thumb|left|200px|Figure 11- Shows the internuclear distance vs time graph of the transition state of the HF + H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reactions]]&lt;br /&gt;
[[File:Screen Shot 2020-05-22 at 11.14.01.png|thumb|200px|Figure 12- This shows the surface plot for the reactions of H+HF and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F. AB distance is showing F approaching H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and BC distance is showing H approaching HF. AB is the distance between F and H and BC is the distance between H and H.]]&lt;br /&gt;
&lt;br /&gt;
====Question 3: Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy can be determined by taking away the energy of the reactants from the transition state energy.&lt;br /&gt;
&lt;br /&gt;
Using LEPS GUI and changing the distances of AB and BC, the energies for the H-F and H-H bonds can be determined. For the H-F bond energy I found to be -560.404 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is similar to -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; which it says in literature. To find this energy, I set the AB distance as 91pm and the BC distance as 4000pm so that the H atom (C) is so far away it doesn&#039;t give any interaction on the HF bond. For the H-H bond energy I found it to be -435.057 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, again this is close to the literature which was -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. To find this energy, I set the AB distance as 4000pm and the BC distance as 74.5pm. &lt;br /&gt;
&lt;br /&gt;
Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--435.057=1.076 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy of HF + H= -433.981--560.404=126.423 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy can also be determined using an MEP calculation and slightly displacing the transition state towards the reactants, this is a more accurate method because in the above method we are assuming that moving the atoms far apart will give us pure reactants.&lt;br /&gt;
&lt;br /&gt;
To determine activation energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the AB distance=182 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a very small drop in the graph and so using the initial and final energies the activation energy can be determined. Figure 13 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--434.144=0.163 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAEpt1118.png|thumb|200px|Figure 13- this shows the energy vs time graph used to calculate the activation energy for the reaction of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
&lt;br /&gt;
To determine activation energy of HF+H, the AB distance=180 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a drop in the graph and so using the two horizontal lines the activation energy can be determined. Figure 14 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of HF + H= -433.981--560.063= 126.082 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAE2pt1118.png|thumb|200px|Figure 14- this shows the energy vs time graph used to calculate the activation energy for the reaction of HF+F.]]&lt;br /&gt;
&lt;br /&gt;
Overall both methods give very similar values for the activation energies of the reactions.&lt;br /&gt;
&lt;br /&gt;
====Question 4: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;br /&gt;
&lt;br /&gt;
Reaction conditions for a reactive trajectory of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F are rHF= AB distance =180 pm, rHH= BC distance = 74 pm, pHF=AB momentum= -1.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and pHH= BC momentum= 0.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The number of steps is 3000. &lt;br /&gt;
&lt;br /&gt;
The energy is conserved, therefore, the potential energy is converted to kinetic energy. This can be seen by the increase in oscillation in figure 15, once the transition state has been overcome and products starting to form. A large amount of the total energy goes to being vibrational energy of the product.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; The product molecule is oscillating lots therefore, can see that this is vibrational energy. Translational energy directs it to get over the potential energy barrier and then it can drop down and the energy becomes vibrational kinetic energy.&lt;br /&gt;
&lt;br /&gt;
[[File:Reactiondynamicspt1118.png|thumb|200px|Figure 15- This is contour plot showing the reaction dynamics of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is BC and F is A.]]&lt;br /&gt;
&lt;br /&gt;
It can be confirmed experimentally as the reactants and products have different vibrational energy states, and so can be tested using IR spectroscopy. It can be checked by looking either at the emission or absorption of the molecules. &lt;br /&gt;
For the reactants all the molecules are in the ground state, when it forms the products some of the molecules are excited, therefore, the some of the products are in the ground state and some in the first excited state. &lt;br /&gt;
When looking at absorption, you can see for the reactants the molecules in the ground state will get excited to the first excited energy level. Therefore, there is only one transition and so there will be only one peak in the IR spectrum. For the products, two transitions can occur, the molecules in the ground state can be excited to the first excited energy level (fundamental transition), and the molecules that are already in the first excited state will be excited to the second excited state (this is an overtone). These two transitions absorb at two different wavelengths. The IR spectrum will now have the same peak as the reactants as well as a peak at a lower wavenumber. This second peak is at a lower wavenumber because the difference between the first and second state is smaller than the difference between the ground state and first excited state, this is due to the anharmonicity of the system. Overtime the intensity of this overtone will decrease and the intensity of the fundamental will increase as molecules fall back down to the ground state. For looking at emission, instead of the molecules being excited they will fall back to the ground state and so light is emitted. This time, the reactant IR will have no peaks as all molecules are already in the ground state. For the products, there will be one peak as the molecules in the first excited state drop back down to the ground state. &lt;br /&gt;
&lt;br /&gt;
Chemiluminescence experiments can be run to study these reactions.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Setup a calculation starting on the side of the reactants of F + H2, at the bottom of the well rHH = 74 pm, with a momentum pFH = -1.0 g.mol-1.pm.fs-1, and explore several values of pHH in the range -6.1 to 6.1 g.mol-1.pm.fs-1 (explore values also close to these limits). What do you observe? &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The initial  rHF distance= 230 pm. A=F B=H C=H&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! pHF/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  pHH/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -6.0 ||-404.014 ||reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule oscillates as it approaches the F atom. At a time when the H atoms in the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule are repelling one another, there is an interaction between the F atom and the H atom (B). The H atom (B) bounces to and fro between the H (C) and F atoms, eventually forms a HF molecule when the other H atom starts to move away. The products oscillate more than the reactants, therefore, they have more vibrational energy.||[[file:row11_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -4.5 || -418.264 ||no reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule moves towards the F atom. The H atom (B) moves towards the F atom and forms the transition state but this atom then bounces back forming H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and moving away. Therefore, the energy barrier is not quite overcome as it rolls back to the reactants.||[[file:row22_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -2.0|| -432.014 ||no reaction||The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule starts to approach the F atom but there is not enough kinetic energy which is vibrational and in the correct direction for the transition state to be reached. The potential energy barrier can not be over come and so it rolls back to the reactants and no reaction occurs.||[[file:row33_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 2.0|| -428.014||no reaction ||This has the same trajectory as above except the molecules have a bit more vibrational energy as it oscillates a bit more. Again there&#039;s still not enough vibrational kinetic energy for the reactants to get over the potential energy barrier and a reaction to occur.||[[file:row44_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 6.0 ||-349.477 ||no reaction || The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; moves towards the F atom and the transition state is achieved. However, no reaction occurs and the molecules roll back to the reactants as opposed to the products. When the transition state is reached the H atom (B) bounces straight back to form the reactants again.||[[file:row55_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;For the same initial position, increase slightly the momentum pFH = -1.6 g.mol-1.pm.fs-1, and considerably reduce the overall energy of the system by reducing the momentum pHH = 0.2 g.mol-1.pm.fs-1. What do you observe now?&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[file:figure16pt1118.png|thumb|200px|Figure 16- This shows the trajectory for the reaction that occurs between H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and F atom, when pBC= pHH = 0.2 g.mol-1.pm.fs-1 and pAB= pFH = -1.6 g.mol-1.pm.fs-1. BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and A is the F atom. ]]&lt;br /&gt;
&lt;br /&gt;
The reaction occurs. The vibrational energy of the products is much greater than that of the reactants, this can be seen in figure 16. This can be seen because the molecules in the product well oscillate more than the molecules in the reactant well. A lot of the potential energy has been converted to vibrational energy. The kinetic energy for this reaction is very low but, the amount of this that is vibrational is enough and in the correct direction in order for the reaction to occur. In this reaction the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F, the transition state is reached. H atom. (B) bounces between the F atom and H atom (C), eventually the H atom (C) moves away and the HF molecule forms.&lt;br /&gt;
&lt;br /&gt;
====Question 5: Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ====&lt;br /&gt;
&lt;br /&gt;
Polyani&#039;s rule is that vibrational energy is able to promote an endothermic reaction more efficiently than translational energy. This is because in an endothermic reaction it is a late transition state and so if translational energy is used to promote the reaction, then it will hit the potential energy barrier and bounce back, the products are higher in energy and so it can not be used to direct to them. Energy needs to be put in to get over the energy barrier. Using translational energy means the incoming atom will hit the molecule and just bounce back, it can&#039;t get over the energy barrier. This energy is not in the correct direction for a reaction to occur. If vibrational energy is used then the molecule will be oscillating in the correct direction for a reaction to take place and can pass over the energy barrier. Therefore, the vibrational energy is more efficient at promoting an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
In an exothermic reaction, translational energy is more efficient than vibrational energy, it has an early transition state. This is because the energy is going down hill. The molecule can now move along the potential energy surface and once it gets to the transition state it can be guided around and move along in the correct direction to form the products. The translational energy directs the reactants to the products. In an exothermic reaction, the transition state is early and so the activation energy is much lower and so easier to get over the potential energy barrier, no energy needs to be put into the system. Therefore, it can just roll down using translational energy and so translational energy is more efficient for this reaction over vibrational energy. For an exothermic reaction, the energy is mainly changed from the translational energy to the vibrational energy of the products.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== References==&lt;br /&gt;
1. K. J. Laidler. Chemical Kinetics. 3rd edition. Harper Collins. 1987&lt;br /&gt;
&lt;br /&gt;
2. Ch301.cm.utexas.edu. 2020. Bond Enthalpies. [online] Available at: &amp;lt;https://ch301.cm.utexas.edu/section2.php?target=thermo/thermochemistry/enthalpy-bonds.html&amp;gt; [Accessed 21 May 2020].&lt;br /&gt;
&lt;br /&gt;
3. Chemistry LibreTexts. 2020. Bond Energies. [online] Available at:&amp;lt;https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Supplemental_Modules_(Physical_and_Theoretical_Chemistry)/Chemical_Bonding/Fundamentals_of_Chemical_Bonding/Bond_Energies&amp;gt; [Accessed 21 May 2020].&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812763</id>
		<title>MRD:01547559</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812763"/>
		<updated>2020-06-04T18:02:58Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Molecular Reaction Dynamics: Applications to triatomic systems- Poppy Tobolski==&lt;br /&gt;
&lt;br /&gt;
===&amp;lt;u&amp;gt;Exercise 1&amp;lt;/u&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
NOTE- r1= BC distance, r2= AB distance, p1= BC momentum, p2= AB momentum. However, it doesn&#039;t matter because this is a symmetrical system.&lt;br /&gt;
&lt;br /&gt;
==== Question 1: On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state resembles that of the reactants or products depending on which it is closer in energy to. In an exothermic reaction, the transition state is closer in energy to the reactants therefore, it resembles that of the reactants over the products. This is an early transition state. In an endothermic reaction the transition state is closer in energy to the products and so the transition state resembles that of the products. This is a late transition state. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|TGood introduction - a reference for Hammonds postulate may help here [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0,  it&#039;s the point where the gradient equals zero. The transition state is at the local maximum within the well of minima, the saddle point. In the surface plot, there is a minimum path that connects the products to the reactants. The transition state can be identified as it is the maxima in this path, this is shown in figure 1. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, the saddle is where the first partial derivative = 0 in both the reaction and orthogonal to the reaction co-ordinates. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
At the transition state, the H atoms do not move because force is a derivative of the potential energy. Therefore, force is zero and so the atoms are stationary.&lt;br /&gt;
&lt;br /&gt;
[[file:transitionstatemaximum_pt1118.png|300px|thumb|Figure 1-This graph is the surface plot for the reaction of H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. In this image, you can see there is a maximum is the minimum energy path, this shows the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|A second derivative will allow you to determine which direction the maxima and minima are in. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
rAB= rBC=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.77pm&lt;br /&gt;
&lt;br /&gt;
When the distance between each of the H atoms equals this the force along the distances is very close to zero. Force is a derivative of the potential energy, and so when it equals zero it means the nuclei in the transition state are zero. It can be seen in figure 2 that the internuclear distance isn&#039;t changing with time when at the transition state, this is because the atoms are stationary.&lt;br /&gt;
&lt;br /&gt;
[[file:forceequalszeropt1118.png|300px|thumb|left|Figure 2-This graph is of the internuclear distance vs time for the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Well described. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 19:02, 4 June 2020 (BST)}}&lt;br /&gt;
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==== Question 3: Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
&lt;br /&gt;
When the MEP calculation is used the path is straight, however, when the dynamic calculation is used the path becomes curved. This is because the molecule is oscillating, but in the MEP calculation this is being ignored. The velocity is zero in the MEP calculation, so the path follows the minima on the valley floor of the product. The MEP calculation is not as realistic as the dynamic calculation, this is because it doesn&#039;t take into account that the atoms have masses and in MEP calculation the molecules have uniform motion. Figures 3 and 4 show this on a contour plot.&lt;br /&gt;
[[file:dynamicpt1118.png|thumb|200px|Figure 3- Contour plot of r1=rts+1 vs r2=rts, dynamic calculation has been used. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:meppt1118.png|thumb|200px|Figure 4- Contour plot of r1=rts+1 vs r2=rts, MEP calculation has been used. A is the approaching H atom and BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Look at the “Internuclear Distances vs Time” and “Momenta vs Time”. What would change if we used the initial conditions r1 = rts and r2 = rts+1 pm instead?&amp;lt;/b&amp;gt;&lt;br /&gt;
When looking at the internuclear distances vs time graph, when you swap r1 and r2 around, the graph follows the same trend except the lines for r1 and r2 change around. This is because now r1 decreases distance slightly as it becomes the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule with time and r2 increases distance with time as the H atom moves away. After about 15 seconds, the reaction has finished as r1 is just oscillating around the H-H bond distance and the other H atom has moved away fully. This is shown by figure 5 and 6. Again for the momenta vs time graph, when you change r1 and r2, the two lines in the graph follow the same trend but they are now swapped over. This is because now p2 increases over time and so the momentum of this H atom moving away increases faster and then plateaus once it has moved fully away and has no attraction to the molecule. For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule the momenta oscillates. This is shown by figure 7 and 8.&lt;br /&gt;
[[file:internuclear1pt1118.png|thumb|200px|Figure 5- Internuclear distance vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:internuclear2pt1118.png|thumb|200px|Figure 6- Internuclear distance vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta1pt1118.png|thumb|200px|Figure 7- Momenta vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta2pt1118.png|thumb|200px|Figure 8- Momenta vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed.&lt;br /&gt;
What do you observe?&amp;lt;/b&amp;gt;&lt;br /&gt;
To get the final positions the &#039;get last geometry&#039; function was used. The final r1=74.04pm, r2=352.59pm, p1=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2=-5.08g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Figures 9 and 10, show the internuclear distance vs time graph and the momenta vs time graph respectively. For the internuclear distance vs time graph the r1 distance increased to a maximum and the r2 distance decreased to a minimum over time. They increased and decreased to the distance at which the transition state is achieved so r1=r2=rts. For the momenta vs time graph, the p2 increased as the H atom approached the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and then reached zero when the transition state was reached again. It continued to increase again as the r2 distance increased again. p1 also increased but in an oscillating fashion, it plateaued when momenta was zero for a bit, when in the transition state, and then over time increased again after the transition state had passed.&lt;br /&gt;
[[file:finalinternuclearpt1118.png|thumb|200px|Figure 9- This is the internuclear distance vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
[[file:finalmomentapt1118.png|thumb|200px|Figure 10- This is the momenta vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
&lt;br /&gt;
====Question 4: Complete the table by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
&lt;br /&gt;
A is the approach H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! p1/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  p2/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 ||-414.280 ||Reactive||The black line shows the reaction dynamics, the AB distance decreases as A approaches BC. The BC distance increases, until the transition state is reached. The reaction occurs and so the transition state is past and AB molecule is formed as C moves away. The black line passes down the product energy valley. ||[[file:row1_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.077 ||no reaction||The black line shows that the AB distance decreases to get to the transition state however, the transition state can not be reached. This is because there&#039;s not enough kinetic energy to get to the transition state and so overcome the energy barrier and form the products and it goes back to the reactants. The black line curves round as A starts to move away from molecule BC again. ||[[file:row2_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1|| -413.977 ||reactive||This reaction dynamic is very similar to the first one. A approaches BC, the AB distance decreases and the BC distance slightly increases therefore, forming the transition state. There&#039;s enough kinetic energy and so the reaction occurs. AB molecule forms and the black line shows this as it travels down the valley of the product energy. ||[[file:row3_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1|| -357.277 ||no reaction  ||From looking at the black line it can be seen that A approaches BC and some interaction forms, the transition state is reached. C still has some attraction to B . B moves between A and C, but goes back to form a molecule with C. The p2 is not large enough for the reaction to continue to form the products. There is enough kinetic energy for the reaction to occur, however, not all this kinetic energy may be as translational energy which is important for the reaction to occur. It is instead vibrational energy of the BC molecule.||[[file:row4_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 ||-349.477 ||reactive ||It can be seen that A moves towards BC and BC distance becomes larger, eventually getting to the transition state. B moves back and forth between A and C forming molecules with both. Eventually, B gets closer to A and further from C and so forming AB molecule, this time p2 is large enough and so the reaction can occur. ||[[file:row5_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
To conclude, in order for a reaction to occur there needs to be enough kinetic energy. Enough of this kinetic energy needs to be translational energy, if all the kinetic energy is vibrational energy of the reactants molecule then the reaction won&#039;t occur. Reaction 1 and 3 show that when p1 is higher the reaction will occur faster. Lastly, p1 and p2 need to both be large enough in order for them to collide and for a reaction to occur as shown by the 4th and 5th set of conditions.&lt;br /&gt;
&lt;br /&gt;
====Question 5: Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
&lt;br /&gt;
Transition state theory assumes that if the reactants have enough energy the transition state will be reached and it will go on to form the products. However, even if there&#039;s enough kinetic energy, then it doesn&#039;t always mean a reaction will occur. This is shown by experimental values. The energy has to be spread correctly, for example as translational energy and not just vibrational energy of the molecule. Therefore, this will decrease the experimental rate because not all the kinetic energy is used as translational energy for the reaction.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Transition state theory also assumes that once you go past the transition state and on to form the products that you cannot go back to form the reactants again. However, in experiment this is possible. Experiment 4 in the table above is an example of this, the reaction doesn&#039;t occur even though the transition state is reached. This also means the experimental rate is lower than predicted as not all the reactants will turn into products even if the transition state is reached.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; &lt;br /&gt;
&lt;br /&gt;
It also assumes that the reaction can be treated classically, but quantum effects do occur in experiment. For example quantum tunnelling, this increases the experimental rate compared to the prediction. &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state theory lastly assumes a quasi-equilibrium between the reactants and transition state.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; How much transition state you get is determined by how much reactant you have and so this determines how much product you will get. However, in experiment there may not be an equilibrium, and therefore, this would mean the experimental rate value would be higher than predicted.&lt;br /&gt;
&lt;br /&gt;
===&amp;lt;u&amp;gt;Exercise 2&amp;lt;/u&amp;gt;===&lt;br /&gt;
 &lt;br /&gt;
====Question 1/2: By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
A= F, B=H, C=H&lt;br /&gt;
&lt;br /&gt;
F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. This reaction is exothermic, the energy of the reactants are higher than that of the products. This is an exothermic reaction because it forms stronger bonds in the products than those which are in the reactants,  it forms HF which has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. More energy is released when the HF bond forms than is needed to break the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond. This also means the transition state will be more similar to the reactants, it is an early transition state. Therefore, the transition state is near to when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the reactant and the minimum pathway on the left (AB) is the product. Therefore, you can see the product energy is lower than the reactant energy and so it&#039;s exothermic.&lt;br /&gt;
The enthalpy change for this reaction is -129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
&lt;br /&gt;
HF+H. This reaction is endothermic, the energy of the reactants are lower than that of the products. HF has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, therefore, energy needs to be put into the reaction to break this bond and so the reaction is endothermic. More energy is needed to break the HF bond than is released when the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond is formed. This means that the transition state will be more similar to the products, it is a late transition state. Therefore, the transition state is near when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the product and the minimum pathway on the left is the reactant. Therefore, you can see the reactant energy is higher than the product energy and so it&#039;s endothermic.&lt;br /&gt;
The enthalpy change for this reaction is 129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
&lt;br /&gt;
Both reactions have the same transition state as they are the same reactions just going in opposite directions. I found the transition by finding where the force equals zero and then checking using the internuclear distances vs time graph to see that the graph was zero. This can be seen in figure 11.&lt;br /&gt;
&lt;br /&gt;
[[file:HHFtspt1118.png|thumb|left|200px|Figure 11- Shows the internuclear distance vs time graph of the transition state of the HF + H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reactions]]&lt;br /&gt;
[[File:Screen Shot 2020-05-22 at 11.14.01.png|thumb|200px|Figure 12- This shows the surface plot for the reactions of H+HF and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F. AB distance is showing F approaching H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and BC distance is showing H approaching HF. AB is the distance between F and H and BC is the distance between H and H.]]&lt;br /&gt;
&lt;br /&gt;
====Question 3: Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy can be determined by taking away the energy of the reactants from the transition state energy.&lt;br /&gt;
&lt;br /&gt;
Using LEPS GUI and changing the distances of AB and BC, the energies for the H-F and H-H bonds can be determined. For the H-F bond energy I found to be -560.404 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is similar to -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; which it says in literature. To find this energy, I set the AB distance as 91pm and the BC distance as 4000pm so that the H atom (C) is so far away it doesn&#039;t give any interaction on the HF bond. For the H-H bond energy I found it to be -435.057 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, again this is close to the literature which was -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. To find this energy, I set the AB distance as 4000pm and the BC distance as 74.5pm. &lt;br /&gt;
&lt;br /&gt;
Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--435.057=1.076 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy of HF + H= -433.981--560.404=126.423 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy can also be determined using an MEP calculation and slightly displacing the transition state towards the reactants, this is a more accurate method because in the above method we are assuming that moving the atoms far apart will give us pure reactants.&lt;br /&gt;
&lt;br /&gt;
To determine activation energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the AB distance=182 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a very small drop in the graph and so using the initial and final energies the activation energy can be determined. Figure 13 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--434.144=0.163 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAEpt1118.png|thumb|200px|Figure 13- this shows the energy vs time graph used to calculate the activation energy for the reaction of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
&lt;br /&gt;
To determine activation energy of HF+H, the AB distance=180 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a drop in the graph and so using the two horizontal lines the activation energy can be determined. Figure 14 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of HF + H= -433.981--560.063= 126.082 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAE2pt1118.png|thumb|200px|Figure 14- this shows the energy vs time graph used to calculate the activation energy for the reaction of HF+F.]]&lt;br /&gt;
&lt;br /&gt;
Overall both methods give very similar values for the activation energies of the reactions.&lt;br /&gt;
&lt;br /&gt;
====Question 4: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;br /&gt;
&lt;br /&gt;
Reaction conditions for a reactive trajectory of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F are rHF= AB distance =180 pm, rHH= BC distance = 74 pm, pHF=AB momentum= -1.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and pHH= BC momentum= 0.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The number of steps is 3000. &lt;br /&gt;
&lt;br /&gt;
The energy is conserved, therefore, the potential energy is converted to kinetic energy. This can be seen by the increase in oscillation in figure 15, once the transition state has been overcome and products starting to form. A large amount of the total energy goes to being vibrational energy of the product.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; The product molecule is oscillating lots therefore, can see that this is vibrational energy. Translational energy directs it to get over the potential energy barrier and then it can drop down and the energy becomes vibrational kinetic energy.&lt;br /&gt;
&lt;br /&gt;
[[File:Reactiondynamicspt1118.png|thumb|200px|Figure 15- This is contour plot showing the reaction dynamics of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is BC and F is A.]]&lt;br /&gt;
&lt;br /&gt;
It can be confirmed experimentally as the reactants and products have different vibrational energy states, and so can be tested using IR spectroscopy. It can be checked by looking either at the emission or absorption of the molecules. &lt;br /&gt;
For the reactants all the molecules are in the ground state, when it forms the products some of the molecules are excited, therefore, the some of the products are in the ground state and some in the first excited state. &lt;br /&gt;
When looking at absorption, you can see for the reactants the molecules in the ground state will get excited to the first excited energy level. Therefore, there is only one transition and so there will be only one peak in the IR spectrum. For the products, two transitions can occur, the molecules in the ground state can be excited to the first excited energy level (fundamental transition), and the molecules that are already in the first excited state will be excited to the second excited state (this is an overtone). These two transitions absorb at two different wavelengths. The IR spectrum will now have the same peak as the reactants as well as a peak at a lower wavenumber. This second peak is at a lower wavenumber because the difference between the first and second state is smaller than the difference between the ground state and first excited state, this is due to the anharmonicity of the system. Overtime the intensity of this overtone will decrease and the intensity of the fundamental will increase as molecules fall back down to the ground state. For looking at emission, instead of the molecules being excited they will fall back to the ground state and so light is emitted. This time, the reactant IR will have no peaks as all molecules are already in the ground state. For the products, there will be one peak as the molecules in the first excited state drop back down to the ground state. &lt;br /&gt;
&lt;br /&gt;
Chemiluminescence experiments can be run to study these reactions.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Setup a calculation starting on the side of the reactants of F + H2, at the bottom of the well rHH = 74 pm, with a momentum pFH = -1.0 g.mol-1.pm.fs-1, and explore several values of pHH in the range -6.1 to 6.1 g.mol-1.pm.fs-1 (explore values also close to these limits). What do you observe? &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The initial  rHF distance= 230 pm. A=F B=H C=H&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! pHF/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  pHH/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -6.0 ||-404.014 ||reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule oscillates as it approaches the F atom. At a time when the H atoms in the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule are repelling one another, there is an interaction between the F atom and the H atom (B). The H atom (B) bounces to and fro between the H (C) and F atoms, eventually forms a HF molecule when the other H atom starts to move away. The products oscillate more than the reactants, therefore, they have more vibrational energy.||[[file:row11_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -4.5 || -418.264 ||no reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule moves towards the F atom. The H atom (B) moves towards the F atom and forms the transition state but this atom then bounces back forming H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and moving away. Therefore, the energy barrier is not quite overcome as it rolls back to the reactants.||[[file:row22_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -2.0|| -432.014 ||no reaction||The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule starts to approach the F atom but there is not enough kinetic energy which is vibrational and in the correct direction for the transition state to be reached. The potential energy barrier can not be over come and so it rolls back to the reactants and no reaction occurs.||[[file:row33_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 2.0|| -428.014||no reaction ||This has the same trajectory as above except the molecules have a bit more vibrational energy as it oscillates a bit more. Again there&#039;s still not enough vibrational kinetic energy for the reactants to get over the potential energy barrier and a reaction to occur.||[[file:row44_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 6.0 ||-349.477 ||no reaction || The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; moves towards the F atom and the transition state is achieved. However, no reaction occurs and the molecules roll back to the reactants as opposed to the products. When the transition state is reached the H atom (B) bounces straight back to form the reactants again.||[[file:row55_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;For the same initial position, increase slightly the momentum pFH = -1.6 g.mol-1.pm.fs-1, and considerably reduce the overall energy of the system by reducing the momentum pHH = 0.2 g.mol-1.pm.fs-1. What do you observe now?&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[file:figure16pt1118.png|thumb|200px|Figure 16- This shows the trajectory for the reaction that occurs between H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and F atom, when pBC= pHH = 0.2 g.mol-1.pm.fs-1 and pAB= pFH = -1.6 g.mol-1.pm.fs-1. BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and A is the F atom. ]]&lt;br /&gt;
&lt;br /&gt;
The reaction occurs. The vibrational energy of the products is much greater than that of the reactants, this can be seen in figure 16. This can be seen because the molecules in the product well oscillate more than the molecules in the reactant well. A lot of the potential energy has been converted to vibrational energy. The kinetic energy for this reaction is very low but, the amount of this that is vibrational is enough and in the correct direction in order for the reaction to occur. In this reaction the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F, the transition state is reached. H atom. (B) bounces between the F atom and H atom (C), eventually the H atom (C) moves away and the HF molecule forms.&lt;br /&gt;
&lt;br /&gt;
====Question 5: Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ====&lt;br /&gt;
&lt;br /&gt;
Polyani&#039;s rule is that vibrational energy is able to promote an endothermic reaction more efficiently than translational energy. This is because in an endothermic reaction it is a late transition state and so if translational energy is used to promote the reaction, then it will hit the potential energy barrier and bounce back, the products are higher in energy and so it can not be used to direct to them. Energy needs to be put in to get over the energy barrier. Using translational energy means the incoming atom will hit the molecule and just bounce back, it can&#039;t get over the energy barrier. This energy is not in the correct direction for a reaction to occur. If vibrational energy is used then the molecule will be oscillating in the correct direction for a reaction to take place and can pass over the energy barrier. Therefore, the vibrational energy is more efficient at promoting an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
In an exothermic reaction, translational energy is more efficient than vibrational energy, it has an early transition state. This is because the energy is going down hill. The molecule can now move along the potential energy surface and once it gets to the transition state it can be guided around and move along in the correct direction to form the products. The translational energy directs the reactants to the products. In an exothermic reaction, the transition state is early and so the activation energy is much lower and so easier to get over the potential energy barrier, no energy needs to be put into the system. Therefore, it can just roll down using translational energy and so translational energy is more efficient for this reaction over vibrational energy. For an exothermic reaction, the energy is mainly changed from the translational energy to the vibrational energy of the products.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== References==&lt;br /&gt;
1. K. J. Laidler. Chemical Kinetics. 3rd edition. Harper Collins. 1987&lt;br /&gt;
&lt;br /&gt;
2. Ch301.cm.utexas.edu. 2020. Bond Enthalpies. [online] Available at: &amp;lt;https://ch301.cm.utexas.edu/section2.php?target=thermo/thermochemistry/enthalpy-bonds.html&amp;gt; [Accessed 21 May 2020].&lt;br /&gt;
&lt;br /&gt;
3. Chemistry LibreTexts. 2020. Bond Energies. [online] Available at:&amp;lt;https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Supplemental_Modules_(Physical_and_Theoretical_Chemistry)/Chemical_Bonding/Fundamentals_of_Chemical_Bonding/Bond_Energies&amp;gt; [Accessed 21 May 2020].&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01547559&amp;diff=812762</id>
		<title>MRD:01547559</title>
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		<updated>2020-06-04T17:58:56Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Question 1: On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? */&lt;/p&gt;
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&lt;div&gt;== Molecular Reaction Dynamics: Applications to triatomic systems- Poppy Tobolski==&lt;br /&gt;
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===&amp;lt;u&amp;gt;Exercise 1&amp;lt;/u&amp;gt;===&lt;br /&gt;
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NOTE- r1= BC distance, r2= AB distance, p1= BC momentum, p2= AB momentum. However, it doesn&#039;t matter because this is a symmetrical system.&lt;br /&gt;
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==== Question 1: On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state resembles that of the reactants or products depending on which it is closer in energy to. In an exothermic reaction, the transition state is closer in energy to the reactants therefore, it resembles that of the reactants over the products. This is an early transition state. In an endothermic reaction the transition state is closer in energy to the products and so the transition state resembles that of the products. This is a late transition state. &lt;br /&gt;
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{{fontcolor1|green|TGood introduction - a reference for Hammonds postulate may help here [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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The transition state is mathematically defined as ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0,  it&#039;s the point where the gradient equals zero. The transition state is at the local maximum within the well of minima, the saddle point. In the surface plot, there is a minimum path that connects the products to the reactants. The transition state can be identified as it is the maxima in this path, this is shown in figure 1. &lt;br /&gt;
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{{fontcolor1|green|Ok, the saddle is where the first partial derivative = 0 in both the reaction and orthogonal to the reaction co-ordinates. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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At the transition state, the H atoms do not move because force is a derivative of the potential energy. Therefore, force is zero and so the atoms are stationary.&lt;br /&gt;
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[[file:transitionstatemaximum_pt1118.png|300px|thumb|Figure 1-This graph is the surface plot for the reaction of H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. In this image, you can see there is a maximum is the minimum energy path, this shows the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
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{{fontcolor1|green|A second derivative will allow you to determine which direction the maxima and minima are in. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 18:58, 4 June 2020 (BST)}}&lt;br /&gt;
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==== Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
rAB= rBC=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.77pm&lt;br /&gt;
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When the distance between each of the H atoms equals this the force along the distances is very close to zero. Force is a derivative of the potential energy, and so when it equals zero it means the nuclei in the transition state are zero. It can be seen in figure 2 that the internuclear distance isn&#039;t changing with time when at the transition state, this is because the atoms are stationary.&lt;br /&gt;
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[[file:forceequalszeropt1118.png|300px|thumb|left|Figure 2-This graph is of the internuclear distance vs time for the transition state. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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==== Question 3: Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
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When the MEP calculation is used the path is straight, however, when the dynamic calculation is used the path becomes curved. This is because the molecule is oscillating, but in the MEP calculation this is being ignored. The velocity is zero in the MEP calculation, so the path follows the minima on the valley floor of the product. The MEP calculation is not as realistic as the dynamic calculation, this is because it doesn&#039;t take into account that the atoms have masses and in MEP calculation the molecules have uniform motion. Figures 3 and 4 show this on a contour plot.&lt;br /&gt;
[[file:dynamicpt1118.png|thumb|200px|Figure 3- Contour plot of r1=rts+1 vs r2=rts, dynamic calculation has been used. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:meppt1118.png|thumb|200px|Figure 4- Contour plot of r1=rts+1 vs r2=rts, MEP calculation has been used. A is the approaching H atom and BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Look at the “Internuclear Distances vs Time” and “Momenta vs Time”. What would change if we used the initial conditions r1 = rts and r2 = rts+1 pm instead?&amp;lt;/b&amp;gt;&lt;br /&gt;
When looking at the internuclear distances vs time graph, when you swap r1 and r2 around, the graph follows the same trend except the lines for r1 and r2 change around. This is because now r1 decreases distance slightly as it becomes the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule with time and r2 increases distance with time as the H atom moves away. After about 15 seconds, the reaction has finished as r1 is just oscillating around the H-H bond distance and the other H atom has moved away fully. This is shown by figure 5 and 6. Again for the momenta vs time graph, when you change r1 and r2, the two lines in the graph follow the same trend but they are now swapped over. This is because now p2 increases over time and so the momentum of this H atom moving away increases faster and then plateaus once it has moved fully away and has no attraction to the molecule. For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule the momenta oscillates. This is shown by figure 7 and 8.&lt;br /&gt;
[[file:internuclear1pt1118.png|thumb|200px|Figure 5- Internuclear distance vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:internuclear2pt1118.png|thumb|200px|Figure 6- Internuclear distance vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta1pt1118.png|thumb|200px|Figure 7- Momenta vs time graph when r1=rts+1 and r2=rts. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
[[file:momenta2pt1118.png|thumb|200px|Figure 8- Momenta vs time graph when r1=rts and r2=rts=1. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed.&lt;br /&gt;
What do you observe?&amp;lt;/b&amp;gt;&lt;br /&gt;
To get the final positions the &#039;get last geometry&#039; function was used. The final r1=74.04pm, r2=352.59pm, p1=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2=-5.08g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Figures 9 and 10, show the internuclear distance vs time graph and the momenta vs time graph respectively. For the internuclear distance vs time graph the r1 distance increased to a maximum and the r2 distance decreased to a minimum over time. They increased and decreased to the distance at which the transition state is achieved so r1=r2=rts. For the momenta vs time graph, the p2 increased as the H atom approached the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and then reached zero when the transition state was reached again. It continued to increase again as the r2 distance increased again. p1 also increased but in an oscillating fashion, it plateaued when momenta was zero for a bit, when in the transition state, and then over time increased again after the transition state had passed.&lt;br /&gt;
[[file:finalinternuclearpt1118.png|thumb|200px|Figure 9- This is the internuclear distance vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule]]&lt;br /&gt;
[[file:finalmomentapt1118.png|thumb|200px|Figure 10- This is the momenta vs time graph when the final positions are put at the initial positions. A is the approaching H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.]]&lt;br /&gt;
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====Question 4: Complete the table by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
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A is the approach H atom and BC the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! p1/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  p2/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 ||-414.280 ||Reactive||The black line shows the reaction dynamics, the AB distance decreases as A approaches BC. The BC distance increases, until the transition state is reached. The reaction occurs and so the transition state is past and AB molecule is formed as C moves away. The black line passes down the product energy valley. ||[[file:row1_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.077 ||no reaction||The black line shows that the AB distance decreases to get to the transition state however, the transition state can not be reached. This is because there&#039;s not enough kinetic energy to get to the transition state and so overcome the energy barrier and form the products and it goes back to the reactants. The black line curves round as A starts to move away from molecule BC again. ||[[file:row2_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1|| -413.977 ||reactive||This reaction dynamic is very similar to the first one. A approaches BC, the AB distance decreases and the BC distance slightly increases therefore, forming the transition state. There&#039;s enough kinetic energy and so the reaction occurs. AB molecule forms and the black line shows this as it travels down the valley of the product energy. ||[[file:row3_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1|| -357.277 ||no reaction  ||From looking at the black line it can be seen that A approaches BC and some interaction forms, the transition state is reached. C still has some attraction to B . B moves between A and C, but goes back to form a molecule with C. The p2 is not large enough for the reaction to continue to form the products. There is enough kinetic energy for the reaction to occur, however, not all this kinetic energy may be as translational energy which is important for the reaction to occur. It is instead vibrational energy of the BC molecule.||[[file:row4_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 ||-349.477 ||reactive ||It can be seen that A moves towards BC and BC distance becomes larger, eventually getting to the transition state. B moves back and forth between A and C forming molecules with both. Eventually, B gets closer to A and further from C and so forming AB molecule, this time p2 is large enough and so the reaction can occur. ||[[file:row5_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
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To conclude, in order for a reaction to occur there needs to be enough kinetic energy. Enough of this kinetic energy needs to be translational energy, if all the kinetic energy is vibrational energy of the reactants molecule then the reaction won&#039;t occur. Reaction 1 and 3 show that when p1 is higher the reaction will occur faster. Lastly, p1 and p2 need to both be large enough in order for them to collide and for a reaction to occur as shown by the 4th and 5th set of conditions.&lt;br /&gt;
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====Question 5: Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
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Transition state theory assumes that if the reactants have enough energy the transition state will be reached and it will go on to form the products. However, even if there&#039;s enough kinetic energy, then it doesn&#039;t always mean a reaction will occur. This is shown by experimental values. The energy has to be spread correctly, for example as translational energy and not just vibrational energy of the molecule. Therefore, this will decrease the experimental rate because not all the kinetic energy is used as translational energy for the reaction.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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Transition state theory also assumes that once you go past the transition state and on to form the products that you cannot go back to form the reactants again. However, in experiment this is possible. Experiment 4 in the table above is an example of this, the reaction doesn&#039;t occur even though the transition state is reached. This also means the experimental rate is lower than predicted as not all the reactants will turn into products even if the transition state is reached.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; &lt;br /&gt;
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It also assumes that the reaction can be treated classically, but quantum effects do occur in experiment. For example quantum tunnelling, this increases the experimental rate compared to the prediction. &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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The transition state theory lastly assumes a quasi-equilibrium between the reactants and transition state.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; How much transition state you get is determined by how much reactant you have and so this determines how much product you will get. However, in experiment there may not be an equilibrium, and therefore, this would mean the experimental rate value would be higher than predicted.&lt;br /&gt;
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===&amp;lt;u&amp;gt;Exercise 2&amp;lt;/u&amp;gt;===&lt;br /&gt;
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====Question 1/2: By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? Locate the approximate position of the transition state.====&lt;br /&gt;
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A= F, B=H, C=H&lt;br /&gt;
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F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. This reaction is exothermic, the energy of the reactants are higher than that of the products. This is an exothermic reaction because it forms stronger bonds in the products than those which are in the reactants,  it forms HF which has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. More energy is released when the HF bond forms than is needed to break the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond. This also means the transition state will be more similar to the reactants, it is an early transition state. Therefore, the transition state is near to when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the reactant and the minimum pathway on the left (AB) is the product. Therefore, you can see the product energy is lower than the reactant energy and so it&#039;s exothermic.&lt;br /&gt;
The enthalpy change for this reaction is -129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
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HF+H. This reaction is endothermic, the energy of the reactants are lower than that of the products. HF has a stronger bond than H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, therefore, energy needs to be put into the reaction to break this bond and so the reaction is endothermic. More energy is needed to break the HF bond than is released when the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; bond is formed. This means that the transition state will be more similar to the products, it is a late transition state. Therefore, the transition state is near when rHF=AB= 180.6pm and rHH=BC= 74.5pm. In figure 12, the minimum pathway on the right (BC) is for the product and the minimum pathway on the left is the reactant. Therefore, you can see the reactant energy is higher than the product energy and so it&#039;s endothermic.&lt;br /&gt;
The enthalpy change for this reaction is 129 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Using the value of -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-H bond energy and -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for the H-F bond energy.&lt;br /&gt;
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Both reactions have the same transition state as they are the same reactions just going in opposite directions. I found the transition by finding where the force equals zero and then checking using the internuclear distances vs time graph to see that the graph was zero. This can be seen in figure 11.&lt;br /&gt;
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[[file:HHFtspt1118.png|thumb|left|200px|Figure 11- Shows the internuclear distance vs time graph of the transition state of the HF + H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reactions]]&lt;br /&gt;
[[File:Screen Shot 2020-05-22 at 11.14.01.png|thumb|200px|Figure 12- This shows the surface plot for the reactions of H+HF and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F. AB distance is showing F approaching H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and BC distance is showing H approaching HF. AB is the distance between F and H and BC is the distance between H and H.]]&lt;br /&gt;
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====Question 3: Report the activation energy for both reactions.====&lt;br /&gt;
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The activation energy can be determined by taking away the energy of the reactants from the transition state energy.&lt;br /&gt;
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Using LEPS GUI and changing the distances of AB and BC, the energies for the H-F and H-H bonds can be determined. For the H-F bond energy I found to be -560.404 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is similar to -565&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; which it says in literature. To find this energy, I set the AB distance as 91pm and the BC distance as 4000pm so that the H atom (C) is so far away it doesn&#039;t give any interaction on the HF bond. For the H-H bond energy I found it to be -435.057 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, again this is close to the literature which was -436&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. To find this energy, I set the AB distance as 4000pm and the BC distance as 74.5pm. &lt;br /&gt;
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Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--435.057=1.076 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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Activation energy of HF + H= -433.981--560.404=126.423 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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The activation energy can also be determined using an MEP calculation and slightly displacing the transition state towards the reactants, this is a more accurate method because in the above method we are assuming that moving the atoms far apart will give us pure reactants.&lt;br /&gt;
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To determine activation energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the AB distance=182 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a very small drop in the graph and so using the initial and final energies the activation energy can be determined. Figure 13 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;= -433.981--434.144=0.163 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAEpt1118.png|thumb|200px|Figure 13- this shows the energy vs time graph used to calculate the activation energy for the reaction of F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
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To determine activation energy of HF+H, the AB distance=180 pm and BC distance =74.5 pm. The number of steps was increased to 4000. There is a drop in the graph and so using the two horizontal lines the activation energy can be determined. Figure 14 shows the energy vs time graph I used.&lt;br /&gt;
Activation energy of HF + H= -433.981--560.063= 126.082 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
[[file:MEPAE2pt1118.png|thumb|200px|Figure 14- this shows the energy vs time graph used to calculate the activation energy for the reaction of HF+F.]]&lt;br /&gt;
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Overall both methods give very similar values for the activation energies of the reactions.&lt;br /&gt;
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====Question 4: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;br /&gt;
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Reaction conditions for a reactive trajectory of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F are rHF= AB distance =180 pm, rHH= BC distance = 74 pm, pHF=AB momentum= -1.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and pHH= BC momentum= 0.3 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The number of steps is 3000. &lt;br /&gt;
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The energy is conserved, therefore, the potential energy is converted to kinetic energy. This can be seen by the increase in oscillation in figure 15, once the transition state has been overcome and products starting to form. A large amount of the total energy goes to being vibrational energy of the product.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; The product molecule is oscillating lots therefore, can see that this is vibrational energy. Translational energy directs it to get over the potential energy barrier and then it can drop down and the energy becomes vibrational kinetic energy.&lt;br /&gt;
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[[File:Reactiondynamicspt1118.png|thumb|200px|Figure 15- This is contour plot showing the reaction dynamics of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is BC and F is A.]]&lt;br /&gt;
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It can be confirmed experimentally as the reactants and products have different vibrational energy states, and so can be tested using IR spectroscopy. It can be checked by looking either at the emission or absorption of the molecules. &lt;br /&gt;
For the reactants all the molecules are in the ground state, when it forms the products some of the molecules are excited, therefore, the some of the products are in the ground state and some in the first excited state. &lt;br /&gt;
When looking at absorption, you can see for the reactants the molecules in the ground state will get excited to the first excited energy level. Therefore, there is only one transition and so there will be only one peak in the IR spectrum. For the products, two transitions can occur, the molecules in the ground state can be excited to the first excited energy level (fundamental transition), and the molecules that are already in the first excited state will be excited to the second excited state (this is an overtone). These two transitions absorb at two different wavelengths. The IR spectrum will now have the same peak as the reactants as well as a peak at a lower wavenumber. This second peak is at a lower wavenumber because the difference between the first and second state is smaller than the difference between the ground state and first excited state, this is due to the anharmonicity of the system. Overtime the intensity of this overtone will decrease and the intensity of the fundamental will increase as molecules fall back down to the ground state. For looking at emission, instead of the molecules being excited they will fall back to the ground state and so light is emitted. This time, the reactant IR will have no peaks as all molecules are already in the ground state. For the products, there will be one peak as the molecules in the first excited state drop back down to the ground state. &lt;br /&gt;
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Chemiluminescence experiments can be run to study these reactions.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Setup a calculation starting on the side of the reactants of F + H2, at the bottom of the well rHH = 74 pm, with a momentum pFH = -1.0 g.mol-1.pm.fs-1, and explore several values of pHH in the range -6.1 to 6.1 g.mol-1.pm.fs-1 (explore values also close to these limits). What do you observe? &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The initial  rHF distance= 230 pm. A=F B=H C=H&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! pHF/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !!  pHH/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics!!	Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -6.0 ||-404.014 ||reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule oscillates as it approaches the F atom. At a time when the H atoms in the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule are repelling one another, there is an interaction between the F atom and the H atom (B). The H atom (B) bounces to and fro between the H (C) and F atoms, eventually forms a HF molecule when the other H atom starts to move away. The products oscillate more than the reactants, therefore, they have more vibrational energy.||[[file:row11_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -4.5 || -418.264 ||no reaction|| The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule moves towards the F atom. The H atom (B) moves towards the F atom and forms the transition state but this atom then bounces back forming H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and moving away. Therefore, the energy barrier is not quite overcome as it rolls back to the reactants.||[[file:row22_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || -2.0|| -432.014 ||no reaction||The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule starts to approach the F atom but there is not enough kinetic energy which is vibrational and in the correct direction for the transition state to be reached. The potential energy barrier can not be over come and so it rolls back to the reactants and no reaction occurs.||[[file:row33_pt1118.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 2.0|| -428.014||no reaction ||This has the same trajectory as above except the molecules have a bit more vibrational energy as it oscillates a bit more. Again there&#039;s still not enough vibrational kinetic energy for the reactants to get over the potential energy barrier and a reaction to occur.||[[file:row44_pt1118.png|200px]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || 6.0 ||-349.477 ||no reaction || The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; moves towards the F atom and the transition state is achieved. However, no reaction occurs and the molecules roll back to the reactants as opposed to the products. When the transition state is reached the H atom (B) bounces straight back to form the reactants again.||[[file:row55_pt1118.png|200px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;For the same initial position, increase slightly the momentum pFH = -1.6 g.mol-1.pm.fs-1, and considerably reduce the overall energy of the system by reducing the momentum pHH = 0.2 g.mol-1.pm.fs-1. What do you observe now?&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[file:figure16pt1118.png|thumb|200px|Figure 16- This shows the trajectory for the reaction that occurs between H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and F atom, when pBC= pHH = 0.2 g.mol-1.pm.fs-1 and pAB= pFH = -1.6 g.mol-1.pm.fs-1. BC is the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and A is the F atom. ]]&lt;br /&gt;
&lt;br /&gt;
The reaction occurs. The vibrational energy of the products is much greater than that of the reactants, this can be seen in figure 16. This can be seen because the molecules in the product well oscillate more than the molecules in the reactant well. A lot of the potential energy has been converted to vibrational energy. The kinetic energy for this reaction is very low but, the amount of this that is vibrational is enough and in the correct direction in order for the reaction to occur. In this reaction the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F, the transition state is reached. H atom. (B) bounces between the F atom and H atom (C), eventually the H atom (C) moves away and the HF molecule forms.&lt;br /&gt;
&lt;br /&gt;
====Question 5: Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. ====&lt;br /&gt;
&lt;br /&gt;
Polyani&#039;s rule is that vibrational energy is able to promote an endothermic reaction more efficiently than translational energy. This is because in an endothermic reaction it is a late transition state and so if translational energy is used to promote the reaction, then it will hit the potential energy barrier and bounce back, the products are higher in energy and so it can not be used to direct to them. Energy needs to be put in to get over the energy barrier. Using translational energy means the incoming atom will hit the molecule and just bounce back, it can&#039;t get over the energy barrier. This energy is not in the correct direction for a reaction to occur. If vibrational energy is used then the molecule will be oscillating in the correct direction for a reaction to take place and can pass over the energy barrier. Therefore, the vibrational energy is more efficient at promoting an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
In an exothermic reaction, translational energy is more efficient than vibrational energy, it has an early transition state. This is because the energy is going down hill. The molecule can now move along the potential energy surface and once it gets to the transition state it can be guided around and move along in the correct direction to form the products. The translational energy directs the reactants to the products. In an exothermic reaction, the transition state is early and so the activation energy is much lower and so easier to get over the potential energy barrier, no energy needs to be put into the system. Therefore, it can just roll down using translational energy and so translational energy is more efficient for this reaction over vibrational energy. For an exothermic reaction, the energy is mainly changed from the translational energy to the vibrational energy of the products.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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== References==&lt;br /&gt;
1. K. J. Laidler. Chemical Kinetics. 3rd edition. Harper Collins. 1987&lt;br /&gt;
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2. Ch301.cm.utexas.edu. 2020. Bond Enthalpies. [online] Available at: &amp;lt;https://ch301.cm.utexas.edu/section2.php?target=thermo/thermochemistry/enthalpy-bonds.html&amp;gt; [Accessed 21 May 2020].&lt;br /&gt;
&lt;br /&gt;
3. Chemistry LibreTexts. 2020. Bond Energies. [online] Available at:&amp;lt;https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Supplemental_Modules_(Physical_and_Theoretical_Chemistry)/Chemical_Bonding/Fundamentals_of_Chemical_Bonding/Bond_Energies&amp;gt; [Accessed 21 May 2020].&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812761</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812761"/>
		<updated>2020-06-04T16:48:12Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Effect of Translational and Vibrational Energy on the Reaction */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
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{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Very well explained. Well done. Please try to refer to figures as you use them in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:16, 4 June 2020 (BST)}}&lt;br /&gt;
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If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
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{{fontcolor1|green|Great introduction [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:19, 4 June 2020 (BST)}}&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great the table is really clearly explained, well done. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:20, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You say half of the cases - where does this information come from? What do you mean by this? &#039;Not light enough&#039; - do you too light to occur? Unclear. Otherwise well answered and plenty of detail [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:23, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, where do those values for bond enthalpies come from? Are they calculated directly or are they referenced? Make sure to make this clear. Question is otherwise well described and good use of figure, again would be much clearer if the figures are reference din the text. I.e. Figure X tells us Y.[[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:25, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, you have used this MEP method again, which has yielded a good result. However, further information is required here. What do the forces along the bond tell us? What about the Hessian matrix? Either of these properties would have allowed you to assess the quality of your estimation. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:26, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|This is a good answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:27, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good answer again, well done. You could have potentially mentioned a calorimetry experiment [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:38, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green| Your explanation here is strong, but could do with a reference for where the information is coming from. You needed to make the argument a bit clearer here. The question was in reference to Polanyi rules which explain the relative early and late TS contributing to a dependency on vibrational or trnaslational energies, this also relates to Hammonds postulate etc.. Setting up the argument around these rules first would have lead to enhanced discussion. You also have framed the example around 4 examples (2 for each reaction direction) and a few more would have helped with the conclusions. It is uncelar what the values of the vibrational energy are (outside of assessing these from the figure), quantitative assessment may have helped the comparison betwen vibrational and translational contributions to the reactivity.[[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:43, 4 June 2020 (BST)}}&lt;br /&gt;
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== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812760</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812760"/>
		<updated>2020-06-04T16:45:01Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Effect of Translational and Vibrational Energy on the Reaction */&lt;/p&gt;
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&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
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{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Very well explained. Well done. Please try to refer to figures as you use them in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:16, 4 June 2020 (BST)}}&lt;br /&gt;
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If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great introduction [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:19, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great the table is really clearly explained, well done. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:20, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You say half of the cases - where does this information come from? What do you mean by this? &#039;Not light enough&#039; - do you too light to occur? Unclear. Otherwise well answered and plenty of detail [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:23, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, where do those values for bond enthalpies come from? Are they calculated directly or are they referenced? Make sure to make this clear. Question is otherwise well described and good use of figure, again would be much clearer if the figures are reference din the text. I.e. Figure X tells us Y.[[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:25, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, you have used this MEP method again, which has yielded a good result. However, further information is required here. What do the forces along the bond tell us? What about the Hessian matrix? Either of these properties would have allowed you to assess the quality of your estimation. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:26, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|This is a good answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:27, 4 June 2020 (BST)}}&lt;br /&gt;
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=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good answer again, well done. You could have potentially mentioned a calorimetry experiment [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:38, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green| You needed to make the argument a bit clearer here. The question was in reference to Polanyi rules. Setting up the argument around these would have lead to enhanced discussion. You also have framed the example around two examples and a few more would have helped with the conclusions. It is uncelar what the values of the vibrational energy are (outside of assessing these from the figure), quantitative assessment may have helped the comparison betwen vibrational and translational contributios.[[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:43, 4 June 2020 (BST)}}&lt;br /&gt;
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== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812759</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812759"/>
		<updated>2020-06-04T16:43:49Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Effect of Translational and Vibrational Energy on the Reaction */&lt;/p&gt;
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&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
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{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Very well explained. Well done. Please try to refer to figures as you use them in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:16, 4 June 2020 (BST)}}&lt;br /&gt;
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If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
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{{fontcolor1|green|Great introduction [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:19, 4 June 2020 (BST)}}&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
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| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
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| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
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| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
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| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
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| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
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&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur.&lt;br /&gt;
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{{fontcolor1|green|Great the table is really clearly explained, well done. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:20, 4 June 2020 (BST)}}&lt;br /&gt;
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=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
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{{fontcolor1|green|You say half of the cases - where does this information come from? What do you mean by this? &#039;Not light enough&#039; - do you too light to occur? Unclear. Otherwise well answered and plenty of detail [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:23, 4 June 2020 (BST)}}&lt;br /&gt;
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== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green| Ok, where do those values for bond enthalpies come from? Are they calculated directly or are they referenced? Make sure to make this clear. Question is otherwise well described and good use of figure, again would be much clearer if the figures are reference din the text. I.e. Figure X tells us Y.[[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:25, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Ok, you have used this MEP method again, which has yielded a good result. However, further information is required here. What do the forces along the bond tell us? What about the Hessian matrix? Either of these properties would have allowed you to assess the quality of your estimation. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:26, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|This is a good answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:27, 4 June 2020 (BST)}}&lt;br /&gt;
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=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Good answer again, well done. You could have potentially mentioned a calorimetry experiment [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:38, 4 June 2020 (BST)}}&lt;br /&gt;
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=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
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For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green| You needed to make the argument a bit clearer here. The question was in reference to Polanyi rules. Setting up the argument around these would have lead to enhanced discussion. You also have framed the example around two examples and a few more would have helped with the conclusions. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:43, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812758</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812758"/>
		<updated>2020-06-04T16:38:40Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Release of Reaction Energy */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Very well explained. Well done. Please try to refer to figures as you use them in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:16, 4 June 2020 (BST)}}&lt;br /&gt;
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If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
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{{fontcolor1|green|Great introduction [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:19, 4 June 2020 (BST)}}&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great the table is really clearly explained, well done. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:20, 4 June 2020 (BST)}}&lt;br /&gt;
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=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You say half of the cases - where does this information come from? What do you mean by this? &#039;Not light enough&#039; - do you too light to occur? Unclear. Otherwise well answered and plenty of detail [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:23, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, where do those values for bond enthalpies come from? Are they calculated directly or are they referenced? Make sure to make this clear. Question is otherwise well described and good use of figure, again would be much clearer if the figures are reference din the text. I.e. Figure X tells us Y.[[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:25, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, you have used this MEP method again, which has yielded a good result. However, further information is required here. What do the forces along the bond tell us? What about the Hessian matrix? Either of these properties would have allowed you to assess the quality of your estimation. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:26, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|This is a good answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:27, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good answer again, well done. You could have potentially mentioned a calorimetry experiment [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:38, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812757</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812757"/>
		<updated>2020-06-04T16:27:26Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* The Activation Energies of the Forward and Backward Reactions */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Very well explained. Well done. Please try to refer to figures as you use them in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:16, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great introduction [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:19, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great the table is really clearly explained, well done. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:20, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You say half of the cases - where does this information come from? What do you mean by this? &#039;Not light enough&#039; - do you too light to occur? Unclear. Otherwise well answered and plenty of detail [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:23, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, where do those values for bond enthalpies come from? Are they calculated directly or are they referenced? Make sure to make this clear. Question is otherwise well described and good use of figure, again would be much clearer if the figures are reference din the text. I.e. Figure X tells us Y.[[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:25, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, you have used this MEP method again, which has yielded a good result. However, further information is required here. What do the forces along the bond tell us? What about the Hessian matrix? Either of these properties would have allowed you to assess the quality of your estimation. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:26, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|This is a good answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:27, 4 June 2020 (BST)}}&lt;br /&gt;
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=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812756</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812756"/>
		<updated>2020-06-04T16:26:32Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* The Transition State of the Transformation */&lt;/p&gt;
&lt;hr /&gt;
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== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
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{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Very well explained. Well done. Please try to refer to figures as you use them in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:16, 4 June 2020 (BST)}}&lt;br /&gt;
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If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
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{{fontcolor1|green|Great introduction [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:19, 4 June 2020 (BST)}}&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great the table is really clearly explained, well done. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:20, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You say half of the cases - where does this information come from? What do you mean by this? &#039;Not light enough&#039; - do you too light to occur? Unclear. Otherwise well answered and plenty of detail [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:23, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, where do those values for bond enthalpies come from? Are they calculated directly or are they referenced? Make sure to make this clear. Question is otherwise well described and good use of figure, again would be much clearer if the figures are reference din the text. I.e. Figure X tells us Y.[[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:25, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, you have used this MEP method again, which has yielded a good result. However, further information is required here. What do the forces along the bond tell us? What about the Hessian matrix? Either of these properties would have allowed you to assess the quality of your estimation. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:26, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812755</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812755"/>
		<updated>2020-06-04T16:25:10Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* The Energetics of the Reactions */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Very well explained. Well done. Please try to refer to figures as you use them in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:16, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great introduction [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:19, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great the table is really clearly explained, well done. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:20, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You say half of the cases - where does this information come from? What do you mean by this? &#039;Not light enough&#039; - do you too light to occur? Unclear. Otherwise well answered and plenty of detail [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:23, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Ok, where do those values for bond enthalpies come from? Are they calculated directly or are they referenced? Make sure to make this clear. Question is otherwise well described and good use of figure, again would be much clearer if the figures are reference din the text. I.e. Figure X tells us Y.[[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:25, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812754</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812754"/>
		<updated>2020-06-04T16:23:47Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Transition State Theory */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Very well explained. Well done. Please try to refer to figures as you use them in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:16, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great introduction [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:19, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great the table is really clearly explained, well done. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:20, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You say half of the cases - where does this information come from? What do you mean by this? &#039;Not light enough&#039; - do you too light to occur? Unclear. Otherwise well answered and plenty of detail [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:23, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812753</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812753"/>
		<updated>2020-06-04T16:20:57Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Testing Different Reaction Trajectories for the Reaction Ha-Hb + Hc -&amp;gt; Ha + Hb-Hc */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
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{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
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=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt;&lt;br /&gt;
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{{fontcolor1|green|Very well explained. Well done. Please try to refer to figures as you use them in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:16, 4 June 2020 (BST)}}&lt;br /&gt;
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If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
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=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
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{{fontcolor1|green|Great introduction [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:19, 4 June 2020 (BST)}}&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
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| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
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| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur.&lt;br /&gt;
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{{fontcolor1|green|Great the table is really clearly explained, well done. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:20, 4 June 2020 (BST)}}&lt;br /&gt;
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=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
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== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812752</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812752"/>
		<updated>2020-06-04T16:19:08Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Testing Different Reaction Trajectories for the Reaction Ha-Hb + Hc -&amp;gt; Ha + Hb-Hc */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Very well explained. Well done. Please try to refer to figures as you use them in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:16, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great introduction [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:19, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur.&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812751</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812751"/>
		<updated>2020-06-04T16:17:22Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* The Minimum Energy Path (MEP) */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Very well explained. Well done. Please try to refer to figures as you use them in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:16, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur. &lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812750</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812750"/>
		<updated>2020-06-04T16:16:53Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* The Minimum Energy Path (MEP) */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Very well explained. Well done. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:16, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur. &lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812749</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812749"/>
		<updated>2020-06-04T16:14:41Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* The Position of the Tranition State for the Reaction H2 + H -&amp;gt; H + H2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what were the initial conditions ? You havnt yet introduced MEP as a concept. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt; If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur. &lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812748</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812748"/>
		<updated>2020-06-04T16:14:14Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* The Position of the Tranition State for the Reaction H2 + H -&amp;gt; H + H2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what were the initial conditions ? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt; If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur. &lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812747</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812747"/>
		<updated>2020-06-04T16:12:41Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* The Position of the Tranition State for the Reaction H2 + H -&amp;gt; H + H2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, what were the initial conditions ? It is unclear how you calculated this. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:12, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt; If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur. &lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812746</id>
		<title>MRD:ML9418</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ML9418&amp;diff=812746"/>
		<updated>2020-06-04T16:02:35Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* The Transition State and its Identification */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Dynamics of the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
=== The Transition State and its Identification ===&lt;br /&gt;
&lt;br /&gt;
The transition state on a potential energy surface diagram is defined as the point where the gradient of the potential ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; is zero in all directions. It is the point with the highest energy on the minimum energy path that connects the reactants and the products. &amp;lt;br&amp;gt; &lt;br /&gt;
For a symmetric potential energy surface, the transition state lies on the diagonal line where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. It is the point on that line with the lowest potential energy. The exact location of the transition state for a reaction with a symmetric potential energy surface can be found by running a minimum energy path simulation starting from a point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. The point where that minimum energy path stops is the transition state. &amp;lt;br&amp;gt; [[File:MRD0158103301.png|frame|thumb|left|Figure 1: potential energy surface plot of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, where the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line is dotted in black and the transition state is circled in red]] &amp;lt;br clear=all&amp;gt;&lt;br /&gt;
A transition state is different from a local minimum due to the fact that it is a saddle point, meaning the surface around it has negative Gaussian curvature. This means that the maximal and minimal values of curvature (the second derivatives) around the transition state are of opposite signs, meaning they curve in opposite directions (up and down). A local minimum, on the other hand, has positive Gaussian curvature, meaning that the curvature is in the same direction all around (up in this case).&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| good use of a figure to illustrate your point. Be careful with your definition here, the saddle is defined as both a minimum (in one reaction) and a maximum (in another orthoganol to the first direction), this relative direction applies to the second partial derivative. Be careful too, in that these derivatives are partial, in that they are with respect to an aspect of the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 17:02, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== The Position of the Tranition State for the Reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
For the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + H -&amp;gt; H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the transition state is at a point where the distances between neighboring hydrogen atoms are around 90.774 pm. This point was found using the method mentioned before - a minimum energy path simulation was run, starting from a point on the diagonal r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. The point where the minimum energy path simulation stops is the transition state, because it is the minimum energy point along the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; line. It can not move any lower (towards the reactants or the products) because at that point the gradient is zero in all directions, including the minimum energy path that connects the reactants and products.&amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103315.png|frame|thumb|left|Figure 2: internuclear distances of hydrogens for the aforementioned reaction plotted against processed steps. This plot was constructed by simulating a minimum energy path from a starting point where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 60 pm]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Minimum Energy Path (MEP) ===&lt;br /&gt;
The minimum energy path, or reaction path is a theoretical reaction trajectory that corresponds to infinitely slow motion of reactants and products. On an MEP, the momenta and velocities are always zero, because the movement of reactants and products is stretched on an infinitely long timescale. The MEP is different from the actual reaction trajectory because on the MEP, the system has no kinetic energy and the potential energy always goes down (unless the MEP is specifically connecting two points on the surface, such as the reactants and the products). This means that the system is always losing total energy to head directly to the point of lowest potential energy. In reality, total energy must always be conserved, so when the trajectory heads downward on the potential energy surface (losing potential energy), it must gain kinetic energy. This can be in the form of translational, rotational, vibrational, or electronic energy. For the given reaction, when an MEP is simulated from a point where r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory heads straight towards the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products along the trough of the valley, whereas when a dynamics simulation is run from the same starting position with 0 momentum, the trajectory clearly shows some vibration between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. This shows that as potential energy is lost, kinetic energy is gained in the form of vibrational energy, in order to conserve total energy.&amp;lt;br&amp;gt; If the simulations were run under the conditions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; + 1 = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 1, the trajectory would lead to the H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; products instead of the H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; products.&amp;lt;br&amp;gt;If the initial and final conditions of the simulations are reversed (initial position on the plot replaced by the final position from the previous simulation, and initial momenta replaced by the final momenta), one ends up with a trajectory that starts from where the previous simulation ended, and ends ar where the previous simulation started. In this case, the trajectory ends exactly at the transition state, and where it starts depends on how many steps the previous simulation was run for. &amp;lt;br&amp;gt;&lt;br /&gt;
[[File:MRD0158103303.png|frame|thumb|left|Figure 3: a comparison of the MEP (right) and the actual reaction path (left) on contour plots, where both paths start from a point that is minimally deviated from the transition state (r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt;+1=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1)]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Testing Different Reaction Trajectories for the Reaction H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; -&amp;gt; H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
Running a reactive simulation for this reaction gives the values of momenta required for the reaction to occur. For r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm, the required value for the momentum p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is between -3.1 and -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the required value for the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. It might seem a fair assumption that all trajectories with the same starting positions, but with higher values of momenta than the minimum required values, would result in the reaction going through to the products, since they would have enough kinetic energy to pass the activation energy barrier. To test this assumption, a table has been constructed where various values for momenta have been tested with the same starting positions r&amp;lt;sub&amp;gt;ab&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;bc&amp;lt;/sub&amp;gt; = 200 pm.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/ kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.28 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches the molecule directly and forms H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, which is vibrationally excited. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once || [[File:MRD0158103304.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -4.1 || -420.08 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches but is unable to displace H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and drifts away from H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path does not cross the activation energy barrier. || [[File:MRD0158103305.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.97 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in a vibrationally excited state, H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier once. || [[File:MRD0158103306.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.2 || No || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then displaces H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier twice. || [[File:Mrd0158103307.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.4 || Yes || H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is in the vibrational ground state. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;, but the repulsion between H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; overcomes the attraction and forces H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; to separate. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; then approaches H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; to produce H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; once again. H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; then approaches and displaces H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; a second time to produce a vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; drifts away from the vibrationally excited H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. Path crosses the activation energy barrier three times. || [[File:MRD0158103308.png|750px]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt; The results from these simulations show that not all trajectories starting from the same positions are reactive, even those that have larger momenta than required. The right combination of momenta is needed for a reaction to occur. &lt;br /&gt;
=== Transition State Theory === &lt;br /&gt;
Transition State Theory tries to predict the rate constant for a reaction based on the properties of the reactants and the structure of the transition state. It is based on an assumption that all trajectories along the reaction coordinate with a kinetic energy higher than the activation energy will be reactive. However, as we determined from the previous tests, it is possible for the reaction trajectory to pass the activation energy barrier to form products briefly, but then cross the barrier once more to form the reactants again. It is even possible for the trajectory to cross the activation energy more times, but in half of these cases, products will not be formed in the end. In those cases, the trajectory is not reactive, even though it has enough kinetic energy to overcome the activation energy barrier. &amp;lt;br&amp;gt;For this reaction, there is also a possibility for the reaction to occur without having enough kinetic energy to pass the barrier. This is possible due to quantum tunneling, which can occur in very light particles. The hydrogen atom, however, is not light enough for this tunnelling to occur frequently enough to overcome the reduction in rate that is caused by the possibility of recrossing the activation energy barrier. The fraction of trajectories that are reactive due to tunnelling is orders of magnitude lower than the fraction of trajectories that are unreactive due to bad momenta combinations. This means that the actual rate of reaction will be smaller than the one determined by Transition State Theory.&amp;lt;br&amp;gt;Another assumption of TST is that a Maxwell-Boltzmann equilibrium is maintained in both the reactants and products. However, in bimolecular gas reactions, such as this one, this does not hold true, since selective energy consumption and release takes place&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Dynamics of the Forward and Backward Reactions of  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H ==&lt;br /&gt;
=== The Energetics of the Reactions ===&lt;br /&gt;
The forward reaction for this transformation is exothermic, whereas the backward reaction is endothermic. This is visible on the surface and contour plots below, as the forward reaction products are lower in potential energy than the reactants. This is because the H-F bond is stronger (565 kJ/Mol) than the H-H bond (432 kJ/mol), making the products HF and H more stable than the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F.&amp;lt;br&amp;gt;[[File:MRD0158103309.png|frame|thumb|left|Figure 4: potential energy surface (left) and contour plot (right) for the reaction, where A is the fluorine atom, and B and C are the hydrogen atoms]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Transition State of the Transformation ===&lt;br /&gt;
The location of the transition state is approximately AB = 181.1 pm and BC = 74.5 pm (distance between hydrogens is 74.5 pm and distance between fluorine and closest hydrogen is 181.1 pm). This value is approximate, since it was found by guessing values until the MEP simulation stayed in approximately the same location for 100 steps of 0.1 fs.&lt;br /&gt;
&amp;lt;br&amp;gt;[[File:MRD0158103310.png|frame|thumb|left|Figure 5: transition state of the reaction displayed on a contour plot]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== The Activation Energies of the Forward and Backward Reactions ===&lt;br /&gt;
The activation energy for the forward reaction is ~1.05 kJ/mol and for the backward reaction it is ~126.67 kJ/mol. These energies were determined by running an MEP simulation from the transition state to the reactants and the products for 8000 steps of 0.2 fs, then estimating where the minimum potential energy plateau would be on an energy against time plot, then subtracting that plateau&#039;s value from the transition state&#039;s potential energy value. A more accurate value for the plateaus could have been determined by running the simulation for at least twice as many steps, but processing that many steps would take a long time. Using this method gives the activation energy for the reactants approaching from infinitely far away. In a solution or container of finite volume, the activation energy would be slightly lower.&amp;lt;br&amp;gt;[[File:MRD0158103311.png|frame|thumb|left|Figure 6: energies plotted against processed steps for going from the transition state to the reactants (left) and to the products (right). This is from an MEP simulation, not a dynamics simulation. The activation energy is the difference between the minimum and maximum energy plateaus]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
=== Release of Reaction Energy ===&lt;br /&gt;
For the forward reaction, which is exothermic, the products have less potential energy than the reactants. Because total energy must always be conserved, this means that the products must have a higher kinetic energy than the reactants. Kinetic energy can be in the form of translational, rotational, vibrational, and electronic energy. In the forward reaction, potential energy is converted to kinetic energy in the form of vibrational motion. This is shown on the figure below.&amp;lt;br&amp;gt;[[File:MRD0158103312.png|frame|thumb|left|Figure 7: contour plot of the forward reaction, where the starting positions are AB = 230 pm, BC = 74 pm, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;]]&amp;lt;br clear=all&amp;gt;To confirm whether the reaction energy is being released vibrationally, one could probe the reaction via IR spectroscopy. If the reaction energy is not converted to vibrational energy, all the product molecules in the reaction would be in the ground state. An IR spectrum, in this situation, would only display the peaks going from the ground state to higher vibrational energy states. However, if the reaction energy does get converted to vibrational energy, some of the molecules would populate higher vibrational energy levels, and an IR spectrum would also show peaks going from the higher energy states to even higher energy states. Those peaks are called hot bands. Since the differences between neighboring energy levels for an anharmonic oscillator become smaller at higher energy levels, an IR spectrum would show smaller hot bands that are slightly shifted to smaller wavenumbers from the main peaks. If many IR spectra were taken throughout the reaction, one would at first see hot bands along with the main peaks, then the hot bands would shrink and the main bands grow as the product molecules relax to the ground state.&amp;lt;br&amp;gt;Another way to determine whether vibrational excitation is occurring is to probe the reaction using infrared chemiluminescence. This is a technique for detecting changes in infrared emission during a reaction, which gives information about the energy states of the products of a reaction&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt;. If infrared radiation is detected from the reaction, it means that potential energy does get converted to vibrational motion. This works because vibrational relaxation, if it is radiative, emits infrared radiation.&amp;lt;br&amp;gt;&lt;br /&gt;
=== Effect of Translational and Vibrational Energy on the Reaction ===&lt;br /&gt;
Running dynamics simulations for the forward and backward reactions using various values for the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reveals some information about whether vibrational or translational motion is needed for each reaction to occur. For the forward reaction, most trajectories that led to products started with the reactants having low vibrational energy. Conversely, for the backward reaction, large vibrational energy was needed to convert reactants to products. For the forward reaction, there was more leeway for choosing the values of momentum than for the backward reaction. Finding a reaction path for the backward reaction proved difficult, as the vibrational motion needed to be just right for the activation energy barrier to be crossed.&amp;lt;br&amp;gt; For the forward reaction, very small values for initial momenta can be used, since the activation energy barrier is very small, whereas the backward reaction needs large momenta to occur. This indicates that the required distribution of kinetic energy between translational and vibrational motion is different in an exothermic reaction and an endothermic reaction.&amp;lt;br&amp;gt;For an exothermic reaction, where the products have a lower potential energy than the reactants, and the activation energy is small, it is better to have less vibrational energy and more translational energy. This is because the activation energy barrier is small and the transition state is directly ahead of the reactants on the potential energy surface plot. This means that the barrier can be easily overcome with enough translational motion, and then the trajectory will just fall into the lower energy products area. Having excess vibrational motion, in this case, could prevent the reaction from occurring because the movement of the vibrational motion on the potential energy surface plot is in a different direction than the minimum energy path. Because of this, excess vibrational energy will cause the trajectory of the reaction to move back and forth up the valley. At the transition state, this can increase the energy barrier that needs to be overcome, and might cause the trajectory to simply fall back towards the products.&lt;br /&gt;
&lt;br /&gt;
For an endothermic reaction, the products have higher potential energy than the reactants and the activation energy is large. On a potential energy surface, the transition state is also not directly ahead of the reactants, but is rather behind the valley&#039;s corner, so approaching it directly requires a very large energy barrier to be overcome. Vibrational motion is more useful in this case because it does not move along the minimum energy path, and if the vibrational motion is timed right, it can more easily overcome the large activation energy barrier. This is because if the timing of the vibrational motion is right, the direction of the trajectory will curve behind the valley&#039;s corner in the exact right way for the trajectory to be heading directly towards the transition state. The effect of these conditions is illustrated on the figures below.&lt;br /&gt;
[[File:MRD0158103313.png|left|frame|Figure 8: an unreactive trajectory (left) with high translational energy but low vibrational energy, and a reactive trajectory (right) with low translational energy but high vibrational energy. These plots are for the endothermic reaction H + HF -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:MRD0158103314.png|left|frame|Figure 9: an unreactive trajectory (left) with high vibrational energy but low translational energy, and a reactive trajectory (right) with low vibrational energy and also low translational energy. These plots are for the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub -&amp;gt; HF + H]]&amp;lt;br clear=all&amp;gt;&lt;br /&gt;
== References ==&lt;br /&gt;
1)Steinfeld, J. I.; Francisco, J. S.; Hase, W. L. Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998. pp. 316-318&amp;lt;br&amp;gt;&lt;br /&gt;
2)A Dictionary of Chemistry, 6th ed.; Oxford University Press, 2008.&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812745</id>
		<title>MRD:Bl1718</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812745"/>
		<updated>2020-06-04T15:15:38Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H-H-H system ==&lt;br /&gt;
=== Dynamics from the transition state region ===&lt;br /&gt;
==== On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
δV(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/δr&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0&lt;br /&gt;
&lt;br /&gt;
Transition state is defined as the derivative of potential energy at a local maximum. To distinguish from a local minimum, you can look at the second derivative of the point, if it is smaller than zero it is a maximum.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful, the transition state is defined by the partial derivatives with respect to the reaction co ordinate and orthoganol to this. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: locating the transition state ===&lt;br /&gt;
==== Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ====&lt;br /&gt;
&lt;br /&gt;
The best estimate of the transition state position is 90.82 pm. &lt;br /&gt;
&lt;br /&gt;
As H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; which means r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. At transition state, the potential energy reaches its maximum while kinetic energy equals to zero. The transition state distance is found by minimizing the force between atoms,as shown in Figure 1.&lt;br /&gt;
&lt;br /&gt;
The &#039; Internuclear Distance vs Time&#039; plot (Figure 2) at 90.82 pm shows a straight line suggesting there is no vibration between atoms.The internuclear distance is constant in time because there is no force at transition state.The kinetic energy is close to zero at this point.&lt;br /&gt;
&lt;br /&gt;
[[File:Setting1bl1718.png |500 px|thumb|center|Figure 1: Setting for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Animation1.png |500 px|thumb|center|Figure 2: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good reference to the figures and correct answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:07, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
==== Comment on how the mep and the trajectory you just calculated differ ====&lt;br /&gt;
&lt;br /&gt;
The graphs of mep are smooth line while all graph of trajectory occur as oscillation. &lt;br /&gt;
This is because dynamic calculation taken atomic mass and phase conditions into account, the energy is converting between kinetic energy and potential energy. Therefore, the inertial motion causes in oscillation on the graph. As for mep, no potential energy is encountered so it shows a smooth trajectory.It is also aware that the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of mep stops at 194 and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of dynamic goes to infinity. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_1.png |600 px|thumb|center|Figure 3: Contour plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_2.png |600 px|thumb|center|Figure 4: Skew plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_3.png |600 px|thumb|center|Figure 5: Surface plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_4.png |600 px|thumb|center|Figure 6: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_5.png |600 px|thumb|center|Figure 7: Internuclear Velocities vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_6.png |600 px|thumb|center|Figure 8: Momenta vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_7.png |600 px|thumb|center|Figure 9: Energy vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
By switching the values of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the shape of the trajectory does not change. This shows that the trajectory is the same for both side of transition state.(Figure 10)&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|There is a lot of information here and your point is therefore hard to understand. Make sure to refer to each figure if you intend to use it to support your discussion. At the moment I cna only see refernece to figures 3 , 4 and 10. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:09, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Reactive and unreactive trajectories ===&lt;br /&gt;
==== Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation7.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The graph shows that the AB distance decreases then bounces back without reaching transition state region. This suggests that there is no product formed.&lt;br /&gt;
|[[File:Animation8.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation9.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The curve line in the plot shows that some products has been formed as it passes through the transition state region, but immediately react backwards to reform reactants.&lt;br /&gt;
|[[File:Animation10.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The curve bounces forwards and backwards in transition state region then go to product region representing the presence of reaction products.&lt;br /&gt;
|[[File:Animation11.png |300px]]&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the reactivity of a reaction is not related to its kinetic energy. Although some systems have enough energy to cross the activation barrier. The reactants can be reformed by recrossing the barrier.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You need to be careful with your comments here. The trajectories account for one combination of the atoms with a given set of momenta, at a given starting PES position. You indicate that some product had formed in the penultimate reaction. This is not the case, the reaction is actually unreactive in total (the product is not formed). The reaction is related to kinetic energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:22, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory ===&lt;br /&gt;
==== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ====&lt;br /&gt;
&lt;br /&gt;
First, the idea of barrier recrossing breaks the assumption of Transition State Theory (TST). TST predictions calculate the rate without counting the recrossing product ,which will overestimate the reaction rate. Second, energy is considered classic in TST while are quantized in molecular level. This will lead to the overestimate calculation in partition functions and activation energy of the system, which will affect the value of reaction rates.&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot;&amp;gt;Chapter 10.3,J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F-H-H system ==&lt;br /&gt;
=== PES inspection ===&lt;br /&gt;
==== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic and H + HF reaction is endothermic. By look at the surface plot of two reactions, the reaction occur with an increase in BC distance and a decrease in AB distance. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy curve starts at a higher value and ends in a lower value, suggesting the reaction is exothermic. For H + HF reaction, the curve starts at a lower value and ends in a high value, suggesting it is endothermic.&lt;br /&gt;
&lt;br /&gt;
In the reaction, if the total energy of bond breaking is higher than the total energy of bond forming, the reaction is exothermic. This suggests that the bond strength of H-H bond in H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is higher than the H-F bond.&lt;br /&gt;
[[File:Surface_Plot1_2.png |500px |thumb|center|Figure 11: A graph of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:Surface_Plot2_2.png |500px |thumb|center|Figure 12: A graph of H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good classification [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:26, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Locate the approximate position of the transition state ====&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 181.10 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 74.49 pm. For H + HF reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 74.49 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 181.10 pm. In both situations, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
This is determined by finding the distance when force equals or closes to zero. As F is a bigger atom, the distance between F and H are expected to be bigger.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot3bl1718.png |500 px|thumb|center|Figure 13: Trajectory for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Surface_Plot4bl1718.png |500 px|thumb|center|Figure 14: Trajectory for H + HF reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good, well described. Please refer to the relevant figures in your text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:29, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Report the activation energy for both reactions ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy at saddle point - energy of reactants.The energy of reactants is determined as the minimum energy by changing r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; while keeping r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; large. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the energy of reactants is -435.100 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy is 1.12 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.  For H + HF reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the energy of reactants is -560.600 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy for H + HF reaction is 126.6 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_8.png |500 px|thumb|center|Figure 15: Reactant energy in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_9.png |500 px|thumb|center|Figure 16: reactant energy in H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good but you need to make it clear how your values relate to your figures here. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 16:00, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Reaction dynamics ===&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally ====&lt;br /&gt;
&lt;br /&gt;
The condition of reaction trajectory is set as the same r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; as its saddle point but a smaller r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;, both momenta are set at zero (i.e. zero initial kinetic energy). From the Animation, the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F atom as it vibrates. At a point, the closer H atom is attracted by F and the formed HF molecule starts to vibrate. The rest H atom gains kinetic energy and repulse from the HF molecule. Since the initial kinetic energy in the system is zero, the Animation shows that some vibrational energy is transferred into kinetic energy. This is also shown in Momenta vs Time plot (Figure 17). The increase in amplitude suggests that a gain in kinetic energy. According to the reference, the reaction is occurred on a highly repulsive surface. When the bimolecule approaches F, the repulsion between Hs causes the closer H atom to recoil, pushing the H atom to F and AB vibration is produced.A schematic representation is also shown in the reference. (Figure 18) &amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the release of energy can be measured by a thermometer. However, it may be hard to measure as the reaction is carried out in gas phase. A more accurate way is to use a bomb calorimetry. The reaction takes place in a sealed container in water. Heat from reaction in the sealed metal container flow to the water. The temperature difference of water can be measured and the heat flow can be determined.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| How does this relate to the energy release? More detail on how to conduct bomb calorimetry would be useful. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 16:11, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
[[File:Animation14bl1718.png |500 px|thumb|center|Figure 17: Momenta vs Time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_11.png |500 px|thumb|center|Figure 18: Schematic representation of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 181.10 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 74.49 pm, so the initial potential energy is the same as its transition state.By increasing the momenta, the kinetic energy of biomolecule increases.From the Contour plots, some curves show the presence of barrier recrossing. This suggests that in translation mode, most released energy is gone to vibration energy causing the increase possibility of barrier recrossing. Whereas in vibration mode, most released energy is gone to translation energy, so the repulsed H atom has more kinetic energy. The  distribution of energy in two difference modes affect the efficiency of reaction. Vibration mode is more efficient than translation mode.&lt;br /&gt;
The position of transition state in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction suggests its surface being a Type-I barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_13.png |500 px|thumb|center|Figure 19: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:bl1718_12.png |500 px|thumb|center|Figure 20: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in H + HF reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 92 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 220 pm.With an increase in p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, the trajectory curve to the product region. This shows with enough translation energy, the reaction can occur. In this system, vibration mode is also more efficient than translation mode. As a reverse of the previous reaction, it is considered to have a late-barrier surface.&amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_14.png |500 px|thumb|center|Figure 21: Contour plots of H + HF reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| I tihnk you needed to make Polanyis rules a bit clearer here. Whilst you are correct r.e. the contribution of different types of energy these required further explaantion within the F-H-H system. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 16:15, 4 June 2020 (BST)}}&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812744</id>
		<title>MRD:Bl1718</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812744"/>
		<updated>2020-06-04T15:11:22Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Reaction dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H-H-H system ==&lt;br /&gt;
=== Dynamics from the transition state region ===&lt;br /&gt;
==== On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
δV(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/δr&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0&lt;br /&gt;
&lt;br /&gt;
Transition state is defined as the derivative of potential energy at a local maximum. To distinguish from a local minimum, you can look at the second derivative of the point, if it is smaller than zero it is a maximum.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful, the transition state is defined by the partial derivatives with respect to the reaction co ordinate and orthoganol to this. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: locating the transition state ===&lt;br /&gt;
==== Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ====&lt;br /&gt;
&lt;br /&gt;
The best estimate of the transition state position is 90.82 pm. &lt;br /&gt;
&lt;br /&gt;
As H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; which means r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. At transition state, the potential energy reaches its maximum while kinetic energy equals to zero. The transition state distance is found by minimizing the force between atoms,as shown in Figure 1.&lt;br /&gt;
&lt;br /&gt;
The &#039; Internuclear Distance vs Time&#039; plot (Figure 2) at 90.82 pm shows a straight line suggesting there is no vibration between atoms.The internuclear distance is constant in time because there is no force at transition state.The kinetic energy is close to zero at this point.&lt;br /&gt;
&lt;br /&gt;
[[File:Setting1bl1718.png |500 px|thumb|center|Figure 1: Setting for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Animation1.png |500 px|thumb|center|Figure 2: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good reference to the figures and correct answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:07, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
==== Comment on how the mep and the trajectory you just calculated differ ====&lt;br /&gt;
&lt;br /&gt;
The graphs of mep are smooth line while all graph of trajectory occur as oscillation. &lt;br /&gt;
This is because dynamic calculation taken atomic mass and phase conditions into account, the energy is converting between kinetic energy and potential energy. Therefore, the inertial motion causes in oscillation on the graph. As for mep, no potential energy is encountered so it shows a smooth trajectory.It is also aware that the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of mep stops at 194 and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of dynamic goes to infinity. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_1.png |600 px|thumb|center|Figure 3: Contour plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_2.png |600 px|thumb|center|Figure 4: Skew plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_3.png |600 px|thumb|center|Figure 5: Surface plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_4.png |600 px|thumb|center|Figure 6: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_5.png |600 px|thumb|center|Figure 7: Internuclear Velocities vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_6.png |600 px|thumb|center|Figure 8: Momenta vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_7.png |600 px|thumb|center|Figure 9: Energy vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
By switching the values of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the shape of the trajectory does not change. This shows that the trajectory is the same for both side of transition state.(Figure 10)&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|There is a lot of information here and your point is therefore hard to understand. Make sure to refer to each figure if you intend to use it to support your discussion. At the moment I cna only see refernece to figures 3 , 4 and 10. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:09, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Reactive and unreactive trajectories ===&lt;br /&gt;
==== Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation7.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The graph shows that the AB distance decreases then bounces back without reaching transition state region. This suggests that there is no product formed.&lt;br /&gt;
|[[File:Animation8.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation9.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The curve line in the plot shows that some products has been formed as it passes through the transition state region, but immediately react backwards to reform reactants.&lt;br /&gt;
|[[File:Animation10.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The curve bounces forwards and backwards in transition state region then go to product region representing the presence of reaction products.&lt;br /&gt;
|[[File:Animation11.png |300px]]&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the reactivity of a reaction is not related to its kinetic energy. Although some systems have enough energy to cross the activation barrier. The reactants can be reformed by recrossing the barrier.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You need to be careful with your comments here. The trajectories account for one combination of the atoms with a given set of momenta, at a given starting PES position. You indicate that some product had formed in the penultimate reaction. This is not the case, the reaction is actually unreactive in total (the product is not formed). The reaction is related to kinetic energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:22, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory ===&lt;br /&gt;
==== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ====&lt;br /&gt;
&lt;br /&gt;
First, the idea of barrier recrossing breaks the assumption of Transition State Theory (TST). TST predictions calculate the rate without counting the recrossing product ,which will overestimate the reaction rate. Second, energy is considered classic in TST while are quantized in molecular level. This will lead to the overestimate calculation in partition functions and activation energy of the system, which will affect the value of reaction rates.&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot;&amp;gt;Chapter 10.3,J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F-H-H system ==&lt;br /&gt;
=== PES inspection ===&lt;br /&gt;
==== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic and H + HF reaction is endothermic. By look at the surface plot of two reactions, the reaction occur with an increase in BC distance and a decrease in AB distance. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy curve starts at a higher value and ends in a lower value, suggesting the reaction is exothermic. For H + HF reaction, the curve starts at a lower value and ends in a high value, suggesting it is endothermic.&lt;br /&gt;
&lt;br /&gt;
In the reaction, if the total energy of bond breaking is higher than the total energy of bond forming, the reaction is exothermic. This suggests that the bond strength of H-H bond in H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is higher than the H-F bond.&lt;br /&gt;
[[File:Surface_Plot1_2.png |500px |thumb|center|Figure 11: A graph of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:Surface_Plot2_2.png |500px |thumb|center|Figure 12: A graph of H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good classification [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:26, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Locate the approximate position of the transition state ====&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 181.10 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 74.49 pm. For H + HF reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 74.49 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 181.10 pm. In both situations, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
This is determined by finding the distance when force equals or closes to zero. As F is a bigger atom, the distance between F and H are expected to be bigger.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot3bl1718.png |500 px|thumb|center|Figure 13: Trajectory for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Surface_Plot4bl1718.png |500 px|thumb|center|Figure 14: Trajectory for H + HF reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good, well described. Please refer to the relevant figures in your text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:29, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Report the activation energy for both reactions ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy at saddle point - energy of reactants.The energy of reactants is determined as the minimum energy by changing r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; while keeping r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; large. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the energy of reactants is -435.100 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy is 1.12 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.  For H + HF reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the energy of reactants is -560.600 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy for H + HF reaction is 126.6 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_8.png |500 px|thumb|center|Figure 15: Reactant energy in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_9.png |500 px|thumb|center|Figure 16: reactant energy in H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good but you need to make it clear how your values relate to your figures here. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 16:00, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Reaction dynamics ===&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally ====&lt;br /&gt;
&lt;br /&gt;
The condition of reaction trajectory is set as the same r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; as its saddle point but a smaller r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;, both momenta are set at zero (i.e. zero initial kinetic energy). From the Animation, the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F atom as it vibrates. At a point, the closer H atom is attracted by F and the formed HF molecule starts to vibrate. The rest H atom gains kinetic energy and repulse from the HF molecule. Since the initial kinetic energy in the system is zero, the Animation shows that some vibrational energy is transferred into kinetic energy. This is also shown in Momenta vs Time plot (Figure 17). The increase in amplitude suggests that a gain in kinetic energy. According to the reference, the reaction is occurred on a highly repulsive surface. When the bimolecule approaches F, the repulsion between Hs causes the closer H atom to recoil, pushing the H atom to F and AB vibration is produced.A schematic representation is also shown in the reference. (Figure 18) &amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the release of energy can be measured by a thermometer. However, it may be hard to measure as the reaction is carried out in gas phase. A more accurate way is to use a bomb calorimetry. The reaction takes place in a sealed container in water. Heat from reaction in the sealed metal container flow to the water. The temperature difference of water can be measured and the heat flow can be determined.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| How does this relate to the energy release? More detail on how to conduct bomb calorimetry would be useful. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 16:11, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
[[File:Animation14bl1718.png |500 px|thumb|center|Figure 17: Momenta vs Time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_11.png |500 px|thumb|center|Figure 18: Schematic representation of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 181.10 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 74.49 pm, so the initial potential energy is the same as its transition state.By increasing the momenta, the kinetic energy of biomolecule increases.From the Contour plots, some curves show the presence of barrier recrossing. This suggests that in translation mode, most released energy is gone to vibration energy causing the increase possibility of barrier recrossing. Whereas in vibration mode, most released energy is gone to translation energy, so the repulsed H atom has more kinetic energy. The  distribution of energy in two difference modes affect the efficiency of reaction. Vibration mode is more efficient than translation mode.&lt;br /&gt;
The position of transition state in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction suggests its surface being a Type-I barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_13.png |500 px|thumb|center|Figure 19: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:bl1718_12.png |500 px|thumb|center|Figure 20: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in H + HF reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 92 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 220 pm.With an increase in p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, the trajectory curve to the product region. This shows with enough translation energy, the reaction can occur. In this system, vibration mode is also more efficient than translation mode. As a reverse of the previous reaction, it is considered to have a late-barrier surface.&amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_14.png |500 px|thumb|center|Figure 21: Contour plots of H + HF reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812741</id>
		<title>MRD:Bl1718</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812741"/>
		<updated>2020-06-04T15:00:10Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Report the activation energy for both reactions */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H-H-H system ==&lt;br /&gt;
=== Dynamics from the transition state region ===&lt;br /&gt;
==== On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
δV(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/δr&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0&lt;br /&gt;
&lt;br /&gt;
Transition state is defined as the derivative of potential energy at a local maximum. To distinguish from a local minimum, you can look at the second derivative of the point, if it is smaller than zero it is a maximum.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful, the transition state is defined by the partial derivatives with respect to the reaction co ordinate and orthoganol to this. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: locating the transition state ===&lt;br /&gt;
==== Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ====&lt;br /&gt;
&lt;br /&gt;
The best estimate of the transition state position is 90.82 pm. &lt;br /&gt;
&lt;br /&gt;
As H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; which means r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. At transition state, the potential energy reaches its maximum while kinetic energy equals to zero. The transition state distance is found by minimizing the force between atoms,as shown in Figure 1.&lt;br /&gt;
&lt;br /&gt;
The &#039; Internuclear Distance vs Time&#039; plot (Figure 2) at 90.82 pm shows a straight line suggesting there is no vibration between atoms.The internuclear distance is constant in time because there is no force at transition state.The kinetic energy is close to zero at this point.&lt;br /&gt;
&lt;br /&gt;
[[File:Setting1bl1718.png |500 px|thumb|center|Figure 1: Setting for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Animation1.png |500 px|thumb|center|Figure 2: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good reference to the figures and correct answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:07, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
==== Comment on how the mep and the trajectory you just calculated differ ====&lt;br /&gt;
&lt;br /&gt;
The graphs of mep are smooth line while all graph of trajectory occur as oscillation. &lt;br /&gt;
This is because dynamic calculation taken atomic mass and phase conditions into account, the energy is converting between kinetic energy and potential energy. Therefore, the inertial motion causes in oscillation on the graph. As for mep, no potential energy is encountered so it shows a smooth trajectory.It is also aware that the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of mep stops at 194 and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of dynamic goes to infinity. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_1.png |600 px|thumb|center|Figure 3: Contour plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_2.png |600 px|thumb|center|Figure 4: Skew plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_3.png |600 px|thumb|center|Figure 5: Surface plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_4.png |600 px|thumb|center|Figure 6: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_5.png |600 px|thumb|center|Figure 7: Internuclear Velocities vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_6.png |600 px|thumb|center|Figure 8: Momenta vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_7.png |600 px|thumb|center|Figure 9: Energy vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
By switching the values of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the shape of the trajectory does not change. This shows that the trajectory is the same for both side of transition state.(Figure 10)&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|There is a lot of information here and your point is therefore hard to understand. Make sure to refer to each figure if you intend to use it to support your discussion. At the moment I cna only see refernece to figures 3 , 4 and 10. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:09, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Reactive and unreactive trajectories ===&lt;br /&gt;
==== Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation7.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The graph shows that the AB distance decreases then bounces back without reaching transition state region. This suggests that there is no product formed.&lt;br /&gt;
|[[File:Animation8.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation9.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The curve line in the plot shows that some products has been formed as it passes through the transition state region, but immediately react backwards to reform reactants.&lt;br /&gt;
|[[File:Animation10.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The curve bounces forwards and backwards in transition state region then go to product region representing the presence of reaction products.&lt;br /&gt;
|[[File:Animation11.png |300px]]&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the reactivity of a reaction is not related to its kinetic energy. Although some systems have enough energy to cross the activation barrier. The reactants can be reformed by recrossing the barrier.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You need to be careful with your comments here. The trajectories account for one combination of the atoms with a given set of momenta, at a given starting PES position. You indicate that some product had formed in the penultimate reaction. This is not the case, the reaction is actually unreactive in total (the product is not formed). The reaction is related to kinetic energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:22, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory ===&lt;br /&gt;
==== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ====&lt;br /&gt;
&lt;br /&gt;
First, the idea of barrier recrossing breaks the assumption of Transition State Theory (TST). TST predictions calculate the rate without counting the recrossing product ,which will overestimate the reaction rate. Second, energy is considered classic in TST while are quantized in molecular level. This will lead to the overestimate calculation in partition functions and activation energy of the system, which will affect the value of reaction rates.&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot;&amp;gt;Chapter 10.3,J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F-H-H system ==&lt;br /&gt;
=== PES inspection ===&lt;br /&gt;
==== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic and H + HF reaction is endothermic. By look at the surface plot of two reactions, the reaction occur with an increase in BC distance and a decrease in AB distance. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy curve starts at a higher value and ends in a lower value, suggesting the reaction is exothermic. For H + HF reaction, the curve starts at a lower value and ends in a high value, suggesting it is endothermic.&lt;br /&gt;
&lt;br /&gt;
In the reaction, if the total energy of bond breaking is higher than the total energy of bond forming, the reaction is exothermic. This suggests that the bond strength of H-H bond in H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is higher than the H-F bond.&lt;br /&gt;
[[File:Surface_Plot1_2.png |500px |thumb|center|Figure 11: A graph of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:Surface_Plot2_2.png |500px |thumb|center|Figure 12: A graph of H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good classification [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:26, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Locate the approximate position of the transition state ====&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 181.10 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 74.49 pm. For H + HF reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 74.49 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 181.10 pm. In both situations, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
This is determined by finding the distance when force equals or closes to zero. As F is a bigger atom, the distance between F and H are expected to be bigger.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot3bl1718.png |500 px|thumb|center|Figure 13: Trajectory for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Surface_Plot4bl1718.png |500 px|thumb|center|Figure 14: Trajectory for H + HF reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good, well described. Please refer to the relevant figures in your text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:29, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Report the activation energy for both reactions ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy at saddle point - energy of reactants.The energy of reactants is determined as the minimum energy by changing r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; while keeping r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; large. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the energy of reactants is -435.100 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy is 1.12 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.  For H + HF reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the energy of reactants is -560.600 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy for H + HF reaction is 126.6 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_8.png |500 px|thumb|center|Figure 15: Reactant energy in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_9.png |500 px|thumb|center|Figure 16: reactant energy in H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good but you need to make it clear how your values relate to your figures here. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 16:00, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Reaction dynamics ===&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally ====&lt;br /&gt;
&lt;br /&gt;
The condition of reaction trajectory is set as the same r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; as its saddle point but a smaller r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;, both momenta are set at zero (i.e. zero initial kinetic energy). From the Animation, the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F atom as it vibrates. At a point, the closer H atom is attracted by F and the formed HF molecule starts to vibrate. The rest H atom gains kinetic energy and repulse from the HF molecule. Since the initial kinetic energy in the system is zero, the Animation shows that some vibrational energy is transferred into kinetic energy. This is also shown in Momenta vs Time plot (Figure 17). The increase in amplitude suggests that a gain in kinetic energy. According to the reference, the reaction is occurred on a highly repulsive surface. When the bimolecule approaches F, the repulsion between Hs causes the closer H atom to recoil, pushing the H atom to F and AB vibration is produced.A schematic representation is also shown in the reference. (Figure 18) &amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the release of energy can be measured by a thermometer. However, it may be hard to measure as the reaction is carried out in gas phase. A more accurate way is to use a bomb calorimetry. The reaction takes place in a sealed container in water. Heat from reaction in the sealed metal container flow to the water. The temperature difference of water can be measured and the heat flow can be determined.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation14bl1718.png |500 px|thumb|center|Figure 17: Momenta vs Time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_11.png |500 px|thumb|center|Figure 18: Schematic representation of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 181.10 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 74.49 pm, so the initial potential energy is the same as its transition state.By increasing the momenta, the kinetic energy of biomolecule increases.From the Contour plots, some curves show the presence of barrier recrossing. This suggests that in translation mode, most released energy is gone to vibration energy causing the increase possibility of barrier recrossing. Whereas in vibration mode, most released energy is gone to translation energy, so the repulsed H atom has more kinetic energy. The  distribution of energy in two difference modes affect the efficiency of reaction. Vibration mode is more efficient than translation mode.&lt;br /&gt;
The position of transition state in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction suggests its surface being a Type-I barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_13.png |500 px|thumb|center|Figure 19: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:bl1718_12.png |500 px|thumb|center|Figure 20: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in H + HF reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 92 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 220 pm.With an increase in p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, the trajectory curve to the product region. This shows with enough translation energy, the reaction can occur. In this system, vibration mode is also more efficient than translation mode. As a reverse of the previous reaction, it is considered to have a late-barrier surface.&amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_14.png |500 px|thumb|center|Figure 21: Contour plots of H + HF reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812740</id>
		<title>MRD:Bl1718</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812740"/>
		<updated>2020-06-04T14:29:36Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Locate the approximate position of the transition state */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H-H-H system ==&lt;br /&gt;
=== Dynamics from the transition state region ===&lt;br /&gt;
==== On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
δV(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/δr&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0&lt;br /&gt;
&lt;br /&gt;
Transition state is defined as the derivative of potential energy at a local maximum. To distinguish from a local minimum, you can look at the second derivative of the point, if it is smaller than zero it is a maximum.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful, the transition state is defined by the partial derivatives with respect to the reaction co ordinate and orthoganol to this. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: locating the transition state ===&lt;br /&gt;
==== Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ====&lt;br /&gt;
&lt;br /&gt;
The best estimate of the transition state position is 90.82 pm. &lt;br /&gt;
&lt;br /&gt;
As H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; which means r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. At transition state, the potential energy reaches its maximum while kinetic energy equals to zero. The transition state distance is found by minimizing the force between atoms,as shown in Figure 1.&lt;br /&gt;
&lt;br /&gt;
The &#039; Internuclear Distance vs Time&#039; plot (Figure 2) at 90.82 pm shows a straight line suggesting there is no vibration between atoms.The internuclear distance is constant in time because there is no force at transition state.The kinetic energy is close to zero at this point.&lt;br /&gt;
&lt;br /&gt;
[[File:Setting1bl1718.png |500 px|thumb|center|Figure 1: Setting for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Animation1.png |500 px|thumb|center|Figure 2: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good reference to the figures and correct answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:07, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
==== Comment on how the mep and the trajectory you just calculated differ ====&lt;br /&gt;
&lt;br /&gt;
The graphs of mep are smooth line while all graph of trajectory occur as oscillation. &lt;br /&gt;
This is because dynamic calculation taken atomic mass and phase conditions into account, the energy is converting between kinetic energy and potential energy. Therefore, the inertial motion causes in oscillation on the graph. As for mep, no potential energy is encountered so it shows a smooth trajectory.It is also aware that the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of mep stops at 194 and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of dynamic goes to infinity. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_1.png |600 px|thumb|center|Figure 3: Contour plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_2.png |600 px|thumb|center|Figure 4: Skew plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_3.png |600 px|thumb|center|Figure 5: Surface plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_4.png |600 px|thumb|center|Figure 6: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_5.png |600 px|thumb|center|Figure 7: Internuclear Velocities vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_6.png |600 px|thumb|center|Figure 8: Momenta vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_7.png |600 px|thumb|center|Figure 9: Energy vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
By switching the values of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the shape of the trajectory does not change. This shows that the trajectory is the same for both side of transition state.(Figure 10)&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|There is a lot of information here and your point is therefore hard to understand. Make sure to refer to each figure if you intend to use it to support your discussion. At the moment I cna only see refernece to figures 3 , 4 and 10. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:09, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Reactive and unreactive trajectories ===&lt;br /&gt;
==== Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation7.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The graph shows that the AB distance decreases then bounces back without reaching transition state region. This suggests that there is no product formed.&lt;br /&gt;
|[[File:Animation8.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation9.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The curve line in the plot shows that some products has been formed as it passes through the transition state region, but immediately react backwards to reform reactants.&lt;br /&gt;
|[[File:Animation10.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The curve bounces forwards and backwards in transition state region then go to product region representing the presence of reaction products.&lt;br /&gt;
|[[File:Animation11.png |300px]]&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the reactivity of a reaction is not related to its kinetic energy. Although some systems have enough energy to cross the activation barrier. The reactants can be reformed by recrossing the barrier.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You need to be careful with your comments here. The trajectories account for one combination of the atoms with a given set of momenta, at a given starting PES position. You indicate that some product had formed in the penultimate reaction. This is not the case, the reaction is actually unreactive in total (the product is not formed). The reaction is related to kinetic energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:22, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory ===&lt;br /&gt;
==== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ====&lt;br /&gt;
&lt;br /&gt;
First, the idea of barrier recrossing breaks the assumption of Transition State Theory (TST). TST predictions calculate the rate without counting the recrossing product ,which will overestimate the reaction rate. Second, energy is considered classic in TST while are quantized in molecular level. This will lead to the overestimate calculation in partition functions and activation energy of the system, which will affect the value of reaction rates.&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot;&amp;gt;Chapter 10.3,J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F-H-H system ==&lt;br /&gt;
=== PES inspection ===&lt;br /&gt;
==== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic and H + HF reaction is endothermic. By look at the surface plot of two reactions, the reaction occur with an increase in BC distance and a decrease in AB distance. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy curve starts at a higher value and ends in a lower value, suggesting the reaction is exothermic. For H + HF reaction, the curve starts at a lower value and ends in a high value, suggesting it is endothermic.&lt;br /&gt;
&lt;br /&gt;
In the reaction, if the total energy of bond breaking is higher than the total energy of bond forming, the reaction is exothermic. This suggests that the bond strength of H-H bond in H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is higher than the H-F bond.&lt;br /&gt;
[[File:Surface_Plot1_2.png |500px |thumb|center|Figure 11: A graph of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:Surface_Plot2_2.png |500px |thumb|center|Figure 12: A graph of H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good classification [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:26, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Locate the approximate position of the transition state ====&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 181.10 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 74.49 pm. For H + HF reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 74.49 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 181.10 pm. In both situations, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
This is determined by finding the distance when force equals or closes to zero. As F is a bigger atom, the distance between F and H are expected to be bigger.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot3bl1718.png |500 px|thumb|center|Figure 13: Trajectory for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Surface_Plot4bl1718.png |500 px|thumb|center|Figure 14: Trajectory for H + HF reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good, well described. Please refer to the relevant figures in your text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:29, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Report the activation energy for both reactions ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy at saddle point - energy of reactants.The energy of reactants is determined as the minimum energy by changing r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; while keeping r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; large. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the energy of reactants is -435.100 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy is 1.12 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.  For H + HF reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the energy of reactants is -560.600 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy for H + HF reaction is 126.6 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_8.png |500 px|thumb|center|Figure 15: Reactant energy in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_9.png |500 px|thumb|center|Figure 16: reactant energy in H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
=== Reaction dynamics ===&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally ====&lt;br /&gt;
&lt;br /&gt;
The condition of reaction trajectory is set as the same r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; as its saddle point but a smaller r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;, both momenta are set at zero (i.e. zero initial kinetic energy). From the Animation, the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F atom as it vibrates. At a point, the closer H atom is attracted by F and the formed HF molecule starts to vibrate. The rest H atom gains kinetic energy and repulse from the HF molecule. Since the initial kinetic energy in the system is zero, the Animation shows that some vibrational energy is transferred into kinetic energy. This is also shown in Momenta vs Time plot (Figure 17). The increase in amplitude suggests that a gain in kinetic energy. According to the reference, the reaction is occurred on a highly repulsive surface. When the bimolecule approaches F, the repulsion between Hs causes the closer H atom to recoil, pushing the H atom to F and AB vibration is produced.A schematic representation is also shown in the reference. (Figure 18) &amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the release of energy can be measured by a thermometer. However, it may be hard to measure as the reaction is carried out in gas phase. A more accurate way is to use a bomb calorimetry. The reaction takes place in a sealed container in water. Heat from reaction in the sealed metal container flow to the water. The temperature difference of water can be measured and the heat flow can be determined.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation14bl1718.png |500 px|thumb|center|Figure 17: Momenta vs Time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_11.png |500 px|thumb|center|Figure 18: Schematic representation of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 181.10 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 74.49 pm, so the initial potential energy is the same as its transition state.By increasing the momenta, the kinetic energy of biomolecule increases.From the Contour plots, some curves show the presence of barrier recrossing. This suggests that in translation mode, most released energy is gone to vibration energy causing the increase possibility of barrier recrossing. Whereas in vibration mode, most released energy is gone to translation energy, so the repulsed H atom has more kinetic energy. The  distribution of energy in two difference modes affect the efficiency of reaction. Vibration mode is more efficient than translation mode.&lt;br /&gt;
The position of transition state in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction suggests its surface being a Type-I barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_13.png |500 px|thumb|center|Figure 19: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:bl1718_12.png |500 px|thumb|center|Figure 20: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in H + HF reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 92 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 220 pm.With an increase in p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, the trajectory curve to the product region. This shows with enough translation energy, the reaction can occur. In this system, vibration mode is also more efficient than translation mode. As a reverse of the previous reaction, it is considered to have a late-barrier surface.&amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_14.png |500 px|thumb|center|Figure 21: Contour plots of H + HF reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812739</id>
		<title>MRD:Bl1718</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812739"/>
		<updated>2020-06-04T14:26:45Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H-H-H system ==&lt;br /&gt;
=== Dynamics from the transition state region ===&lt;br /&gt;
==== On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
δV(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/δr&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0&lt;br /&gt;
&lt;br /&gt;
Transition state is defined as the derivative of potential energy at a local maximum. To distinguish from a local minimum, you can look at the second derivative of the point, if it is smaller than zero it is a maximum.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful, the transition state is defined by the partial derivatives with respect to the reaction co ordinate and orthoganol to this. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: locating the transition state ===&lt;br /&gt;
==== Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ====&lt;br /&gt;
&lt;br /&gt;
The best estimate of the transition state position is 90.82 pm. &lt;br /&gt;
&lt;br /&gt;
As H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; which means r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. At transition state, the potential energy reaches its maximum while kinetic energy equals to zero. The transition state distance is found by minimizing the force between atoms,as shown in Figure 1.&lt;br /&gt;
&lt;br /&gt;
The &#039; Internuclear Distance vs Time&#039; plot (Figure 2) at 90.82 pm shows a straight line suggesting there is no vibration between atoms.The internuclear distance is constant in time because there is no force at transition state.The kinetic energy is close to zero at this point.&lt;br /&gt;
&lt;br /&gt;
[[File:Setting1bl1718.png |500 px|thumb|center|Figure 1: Setting for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Animation1.png |500 px|thumb|center|Figure 2: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good reference to the figures and correct answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:07, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
==== Comment on how the mep and the trajectory you just calculated differ ====&lt;br /&gt;
&lt;br /&gt;
The graphs of mep are smooth line while all graph of trajectory occur as oscillation. &lt;br /&gt;
This is because dynamic calculation taken atomic mass and phase conditions into account, the energy is converting between kinetic energy and potential energy. Therefore, the inertial motion causes in oscillation on the graph. As for mep, no potential energy is encountered so it shows a smooth trajectory.It is also aware that the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of mep stops at 194 and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of dynamic goes to infinity. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_1.png |600 px|thumb|center|Figure 3: Contour plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_2.png |600 px|thumb|center|Figure 4: Skew plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_3.png |600 px|thumb|center|Figure 5: Surface plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_4.png |600 px|thumb|center|Figure 6: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_5.png |600 px|thumb|center|Figure 7: Internuclear Velocities vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_6.png |600 px|thumb|center|Figure 8: Momenta vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_7.png |600 px|thumb|center|Figure 9: Energy vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
By switching the values of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the shape of the trajectory does not change. This shows that the trajectory is the same for both side of transition state.(Figure 10)&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|There is a lot of information here and your point is therefore hard to understand. Make sure to refer to each figure if you intend to use it to support your discussion. At the moment I cna only see refernece to figures 3 , 4 and 10. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:09, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Reactive and unreactive trajectories ===&lt;br /&gt;
==== Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation7.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The graph shows that the AB distance decreases then bounces back without reaching transition state region. This suggests that there is no product formed.&lt;br /&gt;
|[[File:Animation8.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation9.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The curve line in the plot shows that some products has been formed as it passes through the transition state region, but immediately react backwards to reform reactants.&lt;br /&gt;
|[[File:Animation10.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The curve bounces forwards and backwards in transition state region then go to product region representing the presence of reaction products.&lt;br /&gt;
|[[File:Animation11.png |300px]]&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the reactivity of a reaction is not related to its kinetic energy. Although some systems have enough energy to cross the activation barrier. The reactants can be reformed by recrossing the barrier.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You need to be careful with your comments here. The trajectories account for one combination of the atoms with a given set of momenta, at a given starting PES position. You indicate that some product had formed in the penultimate reaction. This is not the case, the reaction is actually unreactive in total (the product is not formed). The reaction is related to kinetic energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:22, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory ===&lt;br /&gt;
==== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ====&lt;br /&gt;
&lt;br /&gt;
First, the idea of barrier recrossing breaks the assumption of Transition State Theory (TST). TST predictions calculate the rate without counting the recrossing product ,which will overestimate the reaction rate. Second, energy is considered classic in TST while are quantized in molecular level. This will lead to the overestimate calculation in partition functions and activation energy of the system, which will affect the value of reaction rates.&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot;&amp;gt;Chapter 10.3,J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F-H-H system ==&lt;br /&gt;
=== PES inspection ===&lt;br /&gt;
==== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic and H + HF reaction is endothermic. By look at the surface plot of two reactions, the reaction occur with an increase in BC distance and a decrease in AB distance. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy curve starts at a higher value and ends in a lower value, suggesting the reaction is exothermic. For H + HF reaction, the curve starts at a lower value and ends in a high value, suggesting it is endothermic.&lt;br /&gt;
&lt;br /&gt;
In the reaction, if the total energy of bond breaking is higher than the total energy of bond forming, the reaction is exothermic. This suggests that the bond strength of H-H bond in H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is higher than the H-F bond.&lt;br /&gt;
[[File:Surface_Plot1_2.png |500px |thumb|center|Figure 11: A graph of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:Surface_Plot2_2.png |500px |thumb|center|Figure 12: A graph of H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Good classification [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:26, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Locate the approximate position of the transition state ====&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 181.10 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 74.49 pm. For H + HF reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 74.49 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 181.10 pm. In both situations, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
This is determined by finding the distance when force equals or closes to zero. As F is a bigger atom, the distance between F and H are expected to be bigger.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot3bl1718.png |500 px|thumb|center|Figure 13: Trajectory for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Surface_Plot4bl1718.png |500 px|thumb|center|Figure 14: Trajectory for H + HF reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
==== Report the activation energy for both reactions ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy at saddle point - energy of reactants.The energy of reactants is determined as the minimum energy by changing r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; while keeping r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; large. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the energy of reactants is -435.100 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy is 1.12 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.  For H + HF reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the energy of reactants is -560.600 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy for H + HF reaction is 126.6 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_8.png |500 px|thumb|center|Figure 15: Reactant energy in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_9.png |500 px|thumb|center|Figure 16: reactant energy in H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
=== Reaction dynamics ===&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally ====&lt;br /&gt;
&lt;br /&gt;
The condition of reaction trajectory is set as the same r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; as its saddle point but a smaller r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;, both momenta are set at zero (i.e. zero initial kinetic energy). From the Animation, the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F atom as it vibrates. At a point, the closer H atom is attracted by F and the formed HF molecule starts to vibrate. The rest H atom gains kinetic energy and repulse from the HF molecule. Since the initial kinetic energy in the system is zero, the Animation shows that some vibrational energy is transferred into kinetic energy. This is also shown in Momenta vs Time plot (Figure 17). The increase in amplitude suggests that a gain in kinetic energy. According to the reference, the reaction is occurred on a highly repulsive surface. When the bimolecule approaches F, the repulsion between Hs causes the closer H atom to recoil, pushing the H atom to F and AB vibration is produced.A schematic representation is also shown in the reference. (Figure 18) &amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the release of energy can be measured by a thermometer. However, it may be hard to measure as the reaction is carried out in gas phase. A more accurate way is to use a bomb calorimetry. The reaction takes place in a sealed container in water. Heat from reaction in the sealed metal container flow to the water. The temperature difference of water can be measured and the heat flow can be determined.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation14bl1718.png |500 px|thumb|center|Figure 17: Momenta vs Time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_11.png |500 px|thumb|center|Figure 18: Schematic representation of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 181.10 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 74.49 pm, so the initial potential energy is the same as its transition state.By increasing the momenta, the kinetic energy of biomolecule increases.From the Contour plots, some curves show the presence of barrier recrossing. This suggests that in translation mode, most released energy is gone to vibration energy causing the increase possibility of barrier recrossing. Whereas in vibration mode, most released energy is gone to translation energy, so the repulsed H atom has more kinetic energy. The  distribution of energy in two difference modes affect the efficiency of reaction. Vibration mode is more efficient than translation mode.&lt;br /&gt;
The position of transition state in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction suggests its surface being a Type-I barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_13.png |500 px|thumb|center|Figure 19: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:bl1718_12.png |500 px|thumb|center|Figure 20: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in H + HF reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 92 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 220 pm.With an increase in p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, the trajectory curve to the product region. This shows with enough translation energy, the reaction can occur. In this system, vibration mode is also more efficient than translation mode. As a reverse of the previous reaction, it is considered to have a late-barrier surface.&amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_14.png |500 px|thumb|center|Figure 21: Contour plots of H + HF reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812737</id>
		<title>MRD:Bl1718</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812737"/>
		<updated>2020-06-04T14:22:15Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H-H-H system ==&lt;br /&gt;
=== Dynamics from the transition state region ===&lt;br /&gt;
==== On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
δV(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/δr&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0&lt;br /&gt;
&lt;br /&gt;
Transition state is defined as the derivative of potential energy at a local maximum. To distinguish from a local minimum, you can look at the second derivative of the point, if it is smaller than zero it is a maximum.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful, the transition state is defined by the partial derivatives with respect to the reaction co ordinate and orthoganol to this. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: locating the transition state ===&lt;br /&gt;
==== Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ====&lt;br /&gt;
&lt;br /&gt;
The best estimate of the transition state position is 90.82 pm. &lt;br /&gt;
&lt;br /&gt;
As H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; which means r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. At transition state, the potential energy reaches its maximum while kinetic energy equals to zero. The transition state distance is found by minimizing the force between atoms,as shown in Figure 1.&lt;br /&gt;
&lt;br /&gt;
The &#039; Internuclear Distance vs Time&#039; plot (Figure 2) at 90.82 pm shows a straight line suggesting there is no vibration between atoms.The internuclear distance is constant in time because there is no force at transition state.The kinetic energy is close to zero at this point.&lt;br /&gt;
&lt;br /&gt;
[[File:Setting1bl1718.png |500 px|thumb|center|Figure 1: Setting for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Animation1.png |500 px|thumb|center|Figure 2: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good reference to the figures and correct answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:07, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
==== Comment on how the mep and the trajectory you just calculated differ ====&lt;br /&gt;
&lt;br /&gt;
The graphs of mep are smooth line while all graph of trajectory occur as oscillation. &lt;br /&gt;
This is because dynamic calculation taken atomic mass and phase conditions into account, the energy is converting between kinetic energy and potential energy. Therefore, the inertial motion causes in oscillation on the graph. As for mep, no potential energy is encountered so it shows a smooth trajectory.It is also aware that the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of mep stops at 194 and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of dynamic goes to infinity. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_1.png |600 px|thumb|center|Figure 3: Contour plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_2.png |600 px|thumb|center|Figure 4: Skew plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_3.png |600 px|thumb|center|Figure 5: Surface plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_4.png |600 px|thumb|center|Figure 6: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_5.png |600 px|thumb|center|Figure 7: Internuclear Velocities vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_6.png |600 px|thumb|center|Figure 8: Momenta vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_7.png |600 px|thumb|center|Figure 9: Energy vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
By switching the values of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the shape of the trajectory does not change. This shows that the trajectory is the same for both side of transition state.(Figure 10)&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|There is a lot of information here and your point is therefore hard to understand. Make sure to refer to each figure if you intend to use it to support your discussion. At the moment I cna only see refernece to figures 3 , 4 and 10. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:09, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Reactive and unreactive trajectories ===&lt;br /&gt;
==== Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation7.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The graph shows that the AB distance decreases then bounces back without reaching transition state region. This suggests that there is no product formed.&lt;br /&gt;
|[[File:Animation8.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation9.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The curve line in the plot shows that some products has been formed as it passes through the transition state region, but immediately react backwards to reform reactants.&lt;br /&gt;
|[[File:Animation10.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The curve bounces forwards and backwards in transition state region then go to product region representing the presence of reaction products.&lt;br /&gt;
|[[File:Animation11.png |300px]]&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the reactivity of a reaction is not related to its kinetic energy. Although some systems have enough energy to cross the activation barrier. The reactants can be reformed by recrossing the barrier.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|You need to be careful with your comments here. The trajectories account for one combination of the atoms with a given set of momenta, at a given starting PES position. You indicate that some product had formed in the penultimate reaction. This is not the case, the reaction is actually unreactive in total (the product is not formed). The reaction is related to kinetic energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 15:22, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory ===&lt;br /&gt;
==== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ====&lt;br /&gt;
&lt;br /&gt;
First, the idea of barrier recrossing breaks the assumption of Transition State Theory (TST). TST predictions calculate the rate without counting the recrossing product ,which will overestimate the reaction rate. Second, energy is considered classic in TST while are quantized in molecular level. This will lead to the overestimate calculation in partition functions and activation energy of the system, which will affect the value of reaction rates.&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot;&amp;gt;Chapter 10.3,J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F-H-H system ==&lt;br /&gt;
=== PES inspection ===&lt;br /&gt;
==== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic and H + HF reaction is endothermic. By look at the surface plot of two reactions, the reaction occur with an increase in BC distance and a decrease in AB distance. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy curve starts at a higher value and ends in a lower value, suggesting the reaction is exothermic. For H + HF reaction, the curve starts at a lower value and ends in a high value, suggesting it is endothermic.&lt;br /&gt;
&lt;br /&gt;
In the reaction, if the total energy of bond breaking is higher than the total energy of bond forming, the reaction is exothermic. This suggests that the bond strength of H-H bond in H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is higher than the H-F bond.&lt;br /&gt;
[[File:Surface_Plot1_2.png |500px |thumb|center|Figure 11: A graph of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:Surface_Plot2_2.png |500px |thumb|center|Figure 12: A graph of H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Locate the approximate position of the transition state ====&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 181.10 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 74.49 pm. For H + HF reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 74.49 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 181.10 pm. In both situations, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
This is determined by finding the distance when force equals or closes to zero. As F is a bigger atom, the distance between F and H are expected to be bigger.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot3bl1718.png |500 px|thumb|center|Figure 13: Trajectory for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Surface_Plot4bl1718.png |500 px|thumb|center|Figure 14: Trajectory for H + HF reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
==== Report the activation energy for both reactions ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy at saddle point - energy of reactants.The energy of reactants is determined as the minimum energy by changing r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; while keeping r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; large. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the energy of reactants is -435.100 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy is 1.12 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.  For H + HF reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the energy of reactants is -560.600 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy for H + HF reaction is 126.6 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_8.png |500 px|thumb|center|Figure 15: Reactant energy in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_9.png |500 px|thumb|center|Figure 16: reactant energy in H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
=== Reaction dynamics ===&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally ====&lt;br /&gt;
&lt;br /&gt;
The condition of reaction trajectory is set as the same r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; as its saddle point but a smaller r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;, both momenta are set at zero (i.e. zero initial kinetic energy). From the Animation, the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F atom as it vibrates. At a point, the closer H atom is attracted by F and the formed HF molecule starts to vibrate. The rest H atom gains kinetic energy and repulse from the HF molecule. Since the initial kinetic energy in the system is zero, the Animation shows that some vibrational energy is transferred into kinetic energy. This is also shown in Momenta vs Time plot (Figure 17). The increase in amplitude suggests that a gain in kinetic energy. According to the reference, the reaction is occurred on a highly repulsive surface. When the bimolecule approaches F, the repulsion between Hs causes the closer H atom to recoil, pushing the H atom to F and AB vibration is produced.A schematic representation is also shown in the reference. (Figure 18) &amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the release of energy can be measured by a thermometer. However, it may be hard to measure as the reaction is carried out in gas phase. A more accurate way is to use a bomb calorimetry. The reaction takes place in a sealed container in water. Heat from reaction in the sealed metal container flow to the water. The temperature difference of water can be measured and the heat flow can be determined.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation14bl1718.png |500 px|thumb|center|Figure 17: Momenta vs Time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_11.png |500 px|thumb|center|Figure 18: Schematic representation of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 181.10 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 74.49 pm, so the initial potential energy is the same as its transition state.By increasing the momenta, the kinetic energy of biomolecule increases.From the Contour plots, some curves show the presence of barrier recrossing. This suggests that in translation mode, most released energy is gone to vibration energy causing the increase possibility of barrier recrossing. Whereas in vibration mode, most released energy is gone to translation energy, so the repulsed H atom has more kinetic energy. The  distribution of energy in two difference modes affect the efficiency of reaction. Vibration mode is more efficient than translation mode.&lt;br /&gt;
The position of transition state in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction suggests its surface being a Type-I barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_13.png |500 px|thumb|center|Figure 19: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:bl1718_12.png |500 px|thumb|center|Figure 20: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in H + HF reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 92 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 220 pm.With an increase in p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, the trajectory curve to the product region. This shows with enough translation energy, the reaction can occur. In this system, vibration mode is also more efficient than translation mode. As a reverse of the previous reaction, it is considered to have a late-barrier surface.&amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_14.png |500 px|thumb|center|Figure 21: Contour plots of H + HF reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812736</id>
		<title>MRD:Bl1718</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812736"/>
		<updated>2020-06-04T13:09:01Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Comment on how the mep and the trajectory you just calculated differ */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H-H-H system ==&lt;br /&gt;
=== Dynamics from the transition state region ===&lt;br /&gt;
==== On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
δV(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/δr&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0&lt;br /&gt;
&lt;br /&gt;
Transition state is defined as the derivative of potential energy at a local maximum. To distinguish from a local minimum, you can look at the second derivative of the point, if it is smaller than zero it is a maximum.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful, the transition state is defined by the partial derivatives with respect to the reaction co ordinate and orthoganol to this. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: locating the transition state ===&lt;br /&gt;
==== Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ====&lt;br /&gt;
&lt;br /&gt;
The best estimate of the transition state position is 90.82 pm. &lt;br /&gt;
&lt;br /&gt;
As H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; which means r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. At transition state, the potential energy reaches its maximum while kinetic energy equals to zero. The transition state distance is found by minimizing the force between atoms,as shown in Figure 1.&lt;br /&gt;
&lt;br /&gt;
The &#039; Internuclear Distance vs Time&#039; plot (Figure 2) at 90.82 pm shows a straight line suggesting there is no vibration between atoms.The internuclear distance is constant in time because there is no force at transition state.The kinetic energy is close to zero at this point.&lt;br /&gt;
&lt;br /&gt;
[[File:Setting1bl1718.png |500 px|thumb|center|Figure 1: Setting for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Animation1.png |500 px|thumb|center|Figure 2: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good reference to the figures and correct answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:07, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
==== Comment on how the mep and the trajectory you just calculated differ ====&lt;br /&gt;
&lt;br /&gt;
The graphs of mep are smooth line while all graph of trajectory occur as oscillation. &lt;br /&gt;
This is because dynamic calculation taken atomic mass and phase conditions into account, the energy is converting between kinetic energy and potential energy. Therefore, the inertial motion causes in oscillation on the graph. As for mep, no potential energy is encountered so it shows a smooth trajectory.It is also aware that the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of mep stops at 194 and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of dynamic goes to infinity. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_1.png |600 px|thumb|center|Figure 3: Contour plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_2.png |600 px|thumb|center|Figure 4: Skew plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_3.png |600 px|thumb|center|Figure 5: Surface plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_4.png |600 px|thumb|center|Figure 6: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_5.png |600 px|thumb|center|Figure 7: Internuclear Velocities vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_6.png |600 px|thumb|center|Figure 8: Momenta vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_7.png |600 px|thumb|center|Figure 9: Energy vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
By switching the values of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the shape of the trajectory does not change. This shows that the trajectory is the same for both side of transition state.(Figure 10)&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|There is a lot of information here and your point is therefore hard to understand. Make sure to refer to each figure if you intend to use it to support your discussion. At the moment I cna only see refernece to figures 3 , 4 and 10. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:09, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Reactive and unreactive trajectories ===&lt;br /&gt;
==== Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation7.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The graph shows that the AB distance decreases then bounces back without reaching transition state region. This suggests that there is no product formed.&lt;br /&gt;
|[[File:Animation8.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation9.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The curve line in the plot shows that some products has been formed as it passes through the transition state region, but immediately react backwards to reform reactants.&lt;br /&gt;
|[[File:Animation10.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The curve bounces forwards and backwards in transition state region then go to product region representing the presence of reaction products.&lt;br /&gt;
|[[File:Animation11.png |300px]]&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the reactivity of a reaction is not related to its kinetic energy. Although some systems have enough energy to cross the activation barrier. The reactants can be reformed by recrossing the barrier.&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory ===&lt;br /&gt;
==== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ====&lt;br /&gt;
&lt;br /&gt;
First, the idea of barrier recrossing breaks the assumption of Transition State Theory (TST). TST predictions calculate the rate without counting the recrossing product ,which will overestimate the reaction rate. Second, energy is considered classic in TST while are quantized in molecular level. This will lead to the overestimate calculation in partition functions and activation energy of the system, which will affect the value of reaction rates.&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot;&amp;gt;Chapter 10.3,J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F-H-H system ==&lt;br /&gt;
=== PES inspection ===&lt;br /&gt;
==== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic and H + HF reaction is endothermic. By look at the surface plot of two reactions, the reaction occur with an increase in BC distance and a decrease in AB distance. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy curve starts at a higher value and ends in a lower value, suggesting the reaction is exothermic. For H + HF reaction, the curve starts at a lower value and ends in a high value, suggesting it is endothermic.&lt;br /&gt;
&lt;br /&gt;
In the reaction, if the total energy of bond breaking is higher than the total energy of bond forming, the reaction is exothermic. This suggests that the bond strength of H-H bond in H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is higher than the H-F bond.&lt;br /&gt;
[[File:Surface_Plot1_2.png |500px |thumb|center|Figure 11: A graph of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:Surface_Plot2_2.png |500px |thumb|center|Figure 12: A graph of H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Locate the approximate position of the transition state ====&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 181.10 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 74.49 pm. For H + HF reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 74.49 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 181.10 pm. In both situations, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
This is determined by finding the distance when force equals or closes to zero. As F is a bigger atom, the distance between F and H are expected to be bigger.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot3bl1718.png |500 px|thumb|center|Figure 13: Trajectory for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Surface_Plot4bl1718.png |500 px|thumb|center|Figure 14: Trajectory for H + HF reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
==== Report the activation energy for both reactions ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy at saddle point - energy of reactants.The energy of reactants is determined as the minimum energy by changing r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; while keeping r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; large. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the energy of reactants is -435.100 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy is 1.12 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.  For H + HF reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the energy of reactants is -560.600 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy for H + HF reaction is 126.6 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_8.png |500 px|thumb|center|Figure 15: Reactant energy in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_9.png |500 px|thumb|center|Figure 16: reactant energy in H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
=== Reaction dynamics ===&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally ====&lt;br /&gt;
&lt;br /&gt;
The condition of reaction trajectory is set as the same r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; as its saddle point but a smaller r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;, both momenta are set at zero (i.e. zero initial kinetic energy). From the Animation, the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F atom as it vibrates. At a point, the closer H atom is attracted by F and the formed HF molecule starts to vibrate. The rest H atom gains kinetic energy and repulse from the HF molecule. Since the initial kinetic energy in the system is zero, the Animation shows that some vibrational energy is transferred into kinetic energy. This is also shown in Momenta vs Time plot (Figure 17). The increase in amplitude suggests that a gain in kinetic energy. According to the reference, the reaction is occurred on a highly repulsive surface. When the bimolecule approaches F, the repulsion between Hs causes the closer H atom to recoil, pushing the H atom to F and AB vibration is produced.A schematic representation is also shown in the reference. (Figure 18) &amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the release of energy can be measured by a thermometer. However, it may be hard to measure as the reaction is carried out in gas phase. A more accurate way is to use a bomb calorimetry. The reaction takes place in a sealed container in water. Heat from reaction in the sealed metal container flow to the water. The temperature difference of water can be measured and the heat flow can be determined.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation14bl1718.png |500 px|thumb|center|Figure 17: Momenta vs Time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_11.png |500 px|thumb|center|Figure 18: Schematic representation of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 181.10 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 74.49 pm, so the initial potential energy is the same as its transition state.By increasing the momenta, the kinetic energy of biomolecule increases.From the Contour plots, some curves show the presence of barrier recrossing. This suggests that in translation mode, most released energy is gone to vibration energy causing the increase possibility of barrier recrossing. Whereas in vibration mode, most released energy is gone to translation energy, so the repulsed H atom has more kinetic energy. The  distribution of energy in two difference modes affect the efficiency of reaction. Vibration mode is more efficient than translation mode.&lt;br /&gt;
The position of transition state in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction suggests its surface being a Type-I barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_13.png |500 px|thumb|center|Figure 19: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:bl1718_12.png |500 px|thumb|center|Figure 20: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in H + HF reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 92 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 220 pm.With an increase in p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, the trajectory curve to the product region. This shows with enough translation energy, the reaction can occur. In this system, vibration mode is also more efficient than translation mode. As a reverse of the previous reaction, it is considered to have a late-barrier surface.&amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_14.png |500 px|thumb|center|Figure 21: Contour plots of H + HF reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812735</id>
		<title>MRD:Bl1718</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812735"/>
		<updated>2020-06-04T13:07:34Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Trajectories from r1 = r2: locating the transition state */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H-H-H system ==&lt;br /&gt;
=== Dynamics from the transition state region ===&lt;br /&gt;
==== On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
δV(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/δr&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0&lt;br /&gt;
&lt;br /&gt;
Transition state is defined as the derivative of potential energy at a local maximum. To distinguish from a local minimum, you can look at the second derivative of the point, if it is smaller than zero it is a maximum.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful, the transition state is defined by the partial derivatives with respect to the reaction co ordinate and orthoganol to this. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: locating the transition state ===&lt;br /&gt;
==== Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ====&lt;br /&gt;
&lt;br /&gt;
The best estimate of the transition state position is 90.82 pm. &lt;br /&gt;
&lt;br /&gt;
As H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; which means r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. At transition state, the potential energy reaches its maximum while kinetic energy equals to zero. The transition state distance is found by minimizing the force between atoms,as shown in Figure 1.&lt;br /&gt;
&lt;br /&gt;
The &#039; Internuclear Distance vs Time&#039; plot (Figure 2) at 90.82 pm shows a straight line suggesting there is no vibration between atoms.The internuclear distance is constant in time because there is no force at transition state.The kinetic energy is close to zero at this point.&lt;br /&gt;
&lt;br /&gt;
[[File:Setting1bl1718.png |500 px|thumb|center|Figure 1: Setting for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Animation1.png |500 px|thumb|center|Figure 2: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Good reference to the figures and correct answer. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:07, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
==== Comment on how the mep and the trajectory you just calculated differ ====&lt;br /&gt;
&lt;br /&gt;
The graphs of mep are smooth line while all graph of trajectory occur as oscillation. &lt;br /&gt;
This is because dynamic calculation taken atomic mass and phase conditions into account, the energy is converting between kinetic energy and potential energy. Therefore, the inertial motion causes in oscillation on the graph. As for mep, no potential energy is encountered so it shows a smooth trajectory.It is also aware that the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of mep stops at 194 and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of dynamic goes to infinity. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_1.png |600 px|thumb|center|Figure 3: Contour plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_2.png |600 px|thumb|center|Figure 4: Skew plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_3.png |600 px|thumb|center|Figure 5: Surface plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_4.png |600 px|thumb|center|Figure 6: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_5.png |600 px|thumb|center|Figure 7: Internuclear Velocities vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_6.png |600 px|thumb|center|Figure 8: Momenta vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_7.png |600 px|thumb|center|Figure 9: Energy vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
By switching the values of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the shape of the trajectory does not change. This shows that the trajectory is the same for both side of transition state.(Figure 10)&lt;br /&gt;
&lt;br /&gt;
=== Reactive and unreactive trajectories ===&lt;br /&gt;
==== Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation7.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The graph shows that the AB distance decreases then bounces back without reaching transition state region. This suggests that there is no product formed.&lt;br /&gt;
|[[File:Animation8.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation9.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The curve line in the plot shows that some products has been formed as it passes through the transition state region, but immediately react backwards to reform reactants.&lt;br /&gt;
|[[File:Animation10.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The curve bounces forwards and backwards in transition state region then go to product region representing the presence of reaction products.&lt;br /&gt;
|[[File:Animation11.png |300px]]&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the reactivity of a reaction is not related to its kinetic energy. Although some systems have enough energy to cross the activation barrier. The reactants can be reformed by recrossing the barrier.&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory ===&lt;br /&gt;
==== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ====&lt;br /&gt;
&lt;br /&gt;
First, the idea of barrier recrossing breaks the assumption of Transition State Theory (TST). TST predictions calculate the rate without counting the recrossing product ,which will overestimate the reaction rate. Second, energy is considered classic in TST while are quantized in molecular level. This will lead to the overestimate calculation in partition functions and activation energy of the system, which will affect the value of reaction rates.&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot;&amp;gt;Chapter 10.3,J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F-H-H system ==&lt;br /&gt;
=== PES inspection ===&lt;br /&gt;
==== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic and H + HF reaction is endothermic. By look at the surface plot of two reactions, the reaction occur with an increase in BC distance and a decrease in AB distance. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy curve starts at a higher value and ends in a lower value, suggesting the reaction is exothermic. For H + HF reaction, the curve starts at a lower value and ends in a high value, suggesting it is endothermic.&lt;br /&gt;
&lt;br /&gt;
In the reaction, if the total energy of bond breaking is higher than the total energy of bond forming, the reaction is exothermic. This suggests that the bond strength of H-H bond in H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is higher than the H-F bond.&lt;br /&gt;
[[File:Surface_Plot1_2.png |500px |thumb|center|Figure 11: A graph of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:Surface_Plot2_2.png |500px |thumb|center|Figure 12: A graph of H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Locate the approximate position of the transition state ====&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 181.10 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 74.49 pm. For H + HF reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 74.49 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 181.10 pm. In both situations, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
This is determined by finding the distance when force equals or closes to zero. As F is a bigger atom, the distance between F and H are expected to be bigger.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot3bl1718.png |500 px|thumb|center|Figure 13: Trajectory for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Surface_Plot4bl1718.png |500 px|thumb|center|Figure 14: Trajectory for H + HF reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
==== Report the activation energy for both reactions ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy at saddle point - energy of reactants.The energy of reactants is determined as the minimum energy by changing r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; while keeping r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; large. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the energy of reactants is -435.100 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy is 1.12 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.  For H + HF reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the energy of reactants is -560.600 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy for H + HF reaction is 126.6 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_8.png |500 px|thumb|center|Figure 15: Reactant energy in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_9.png |500 px|thumb|center|Figure 16: reactant energy in H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
=== Reaction dynamics ===&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally ====&lt;br /&gt;
&lt;br /&gt;
The condition of reaction trajectory is set as the same r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; as its saddle point but a smaller r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;, both momenta are set at zero (i.e. zero initial kinetic energy). From the Animation, the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F atom as it vibrates. At a point, the closer H atom is attracted by F and the formed HF molecule starts to vibrate. The rest H atom gains kinetic energy and repulse from the HF molecule. Since the initial kinetic energy in the system is zero, the Animation shows that some vibrational energy is transferred into kinetic energy. This is also shown in Momenta vs Time plot (Figure 17). The increase in amplitude suggests that a gain in kinetic energy. According to the reference, the reaction is occurred on a highly repulsive surface. When the bimolecule approaches F, the repulsion between Hs causes the closer H atom to recoil, pushing the H atom to F and AB vibration is produced.A schematic representation is also shown in the reference. (Figure 18) &amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the release of energy can be measured by a thermometer. However, it may be hard to measure as the reaction is carried out in gas phase. A more accurate way is to use a bomb calorimetry. The reaction takes place in a sealed container in water. Heat from reaction in the sealed metal container flow to the water. The temperature difference of water can be measured and the heat flow can be determined.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation14bl1718.png |500 px|thumb|center|Figure 17: Momenta vs Time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_11.png |500 px|thumb|center|Figure 18: Schematic representation of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 181.10 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 74.49 pm, so the initial potential energy is the same as its transition state.By increasing the momenta, the kinetic energy of biomolecule increases.From the Contour plots, some curves show the presence of barrier recrossing. This suggests that in translation mode, most released energy is gone to vibration energy causing the increase possibility of barrier recrossing. Whereas in vibration mode, most released energy is gone to translation energy, so the repulsed H atom has more kinetic energy. The  distribution of energy in two difference modes affect the efficiency of reaction. Vibration mode is more efficient than translation mode.&lt;br /&gt;
The position of transition state in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction suggests its surface being a Type-I barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_13.png |500 px|thumb|center|Figure 19: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:bl1718_12.png |500 px|thumb|center|Figure 20: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in H + HF reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 92 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 220 pm.With an increase in p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, the trajectory curve to the product region. This shows with enough translation energy, the reaction can occur. In this system, vibration mode is also more efficient than translation mode. As a reverse of the previous reaction, it is considered to have a late-barrier surface.&amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_14.png |500 px|thumb|center|Figure 21: Contour plots of H + HF reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812734</id>
		<title>MRD:Bl1718</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Bl1718&amp;diff=812734"/>
		<updated>2020-06-04T13:04:37Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H-H-H system ==&lt;br /&gt;
=== Dynamics from the transition state region ===&lt;br /&gt;
==== On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ====&lt;br /&gt;
δV(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/δr&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0&lt;br /&gt;
&lt;br /&gt;
Transition state is defined as the derivative of potential energy at a local maximum. To distinguish from a local minimum, you can look at the second derivative of the point, if it is smaller than zero it is a maximum.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Be careful, the transition state is defined by the partial derivatives with respect to the reaction co ordinate and orthoganol to this. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 14:04, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: locating the transition state ===&lt;br /&gt;
==== Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ====&lt;br /&gt;
&lt;br /&gt;
The best estimate of the transition state position is 90.82 pm. &lt;br /&gt;
&lt;br /&gt;
As H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; which means r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. At transition state, the potential energy reaches its maximum while kinetic energy equals to zero. The transition state distance is found by minimizing the force between atoms,as shown in Figure 1.&lt;br /&gt;
&lt;br /&gt;
The &#039; Internuclear Distance vs Time&#039; plot (Figure 2) at 90.82 pm shows a straight line suggesting there is no vibration between atoms.The internuclear distance is constant in time because there is no force at transition state.The kinetic energy is close to zero at this point.&lt;br /&gt;
&lt;br /&gt;
[[File:Setting1bl1718.png |500 px|thumb|center|Figure 1: Setting for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Animation1.png |500 px|thumb|center|Figure 2: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
=== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
==== Comment on how the mep and the trajectory you just calculated differ ====&lt;br /&gt;
&lt;br /&gt;
The graphs of mep are smooth line while all graph of trajectory occur as oscillation. &lt;br /&gt;
This is because dynamic calculation taken atomic mass and phase conditions into account, the energy is converting between kinetic energy and potential energy. Therefore, the inertial motion causes in oscillation on the graph. As for mep, no potential energy is encountered so it shows a smooth trajectory.It is also aware that the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of mep stops at 194 and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; of dynamic goes to infinity. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_1.png |600 px|thumb|center|Figure 3: Contour plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_2.png |600 px|thumb|center|Figure 4: Skew plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_3.png |600 px|thumb|center|Figure 5: Surface plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_4.png |600 px|thumb|center|Figure 6: Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_5.png |600 px|thumb|center|Figure 7: Internuclear Velocities vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_6.png |600 px|thumb|center|Figure 8: Momenta vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_7.png |600 px|thumb|center|Figure 9: Energy vs Time for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
By switching the values of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the shape of the trajectory does not change. This shows that the trajectory is the same for both side of transition state.(Figure 10)&lt;br /&gt;
&lt;br /&gt;
=== Reactive and unreactive trajectories ===&lt;br /&gt;
==== Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table? ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation7.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The graph shows that the AB distance decreases then bounces back without reaching transition state region. This suggests that there is no product formed.&lt;br /&gt;
|[[File:Animation8.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The reaction curve smoothly passes through transition state region then go to the product side showing reaction products are formed and the reaction is occurring.&lt;br /&gt;
|[[File:Animation9.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The curve line in the plot shows that some products has been formed as it passes through the transition state region, but immediately react backwards to reform reactants.&lt;br /&gt;
|[[File:Animation10.png |300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The curve bounces forwards and backwards in transition state region then go to product region representing the presence of reaction products.&lt;br /&gt;
|[[File:Animation11.png |300px]]&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the reactivity of a reaction is not related to its kinetic energy. Although some systems have enough energy to cross the activation barrier. The reactants can be reformed by recrossing the barrier.&lt;br /&gt;
&lt;br /&gt;
=== Transition State Theory ===&lt;br /&gt;
==== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ====&lt;br /&gt;
&lt;br /&gt;
First, the idea of barrier recrossing breaks the assumption of Transition State Theory (TST). TST predictions calculate the rate without counting the recrossing product ,which will overestimate the reaction rate. Second, energy is considered classic in TST while are quantized in molecular level. This will lead to the overestimate calculation in partition functions and activation energy of the system, which will affect the value of reaction rates.&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot; Chemical Kinetic and Dynamics&amp;quot;&amp;gt;Chapter 10.3,J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F-H-H system ==&lt;br /&gt;
=== PES inspection ===&lt;br /&gt;
==== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic and H + HF reaction is endothermic. By look at the surface plot of two reactions, the reaction occur with an increase in BC distance and a decrease in AB distance. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy curve starts at a higher value and ends in a lower value, suggesting the reaction is exothermic. For H + HF reaction, the curve starts at a lower value and ends in a high value, suggesting it is endothermic.&lt;br /&gt;
&lt;br /&gt;
In the reaction, if the total energy of bond breaking is higher than the total energy of bond forming, the reaction is exothermic. This suggests that the bond strength of H-H bond in H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is higher than the H-F bond.&lt;br /&gt;
[[File:Surface_Plot1_2.png |500px |thumb|center|Figure 11: A graph of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:Surface_Plot2_2.png |500px |thumb|center|Figure 12: A graph of H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Locate the approximate position of the transition state ====&lt;br /&gt;
For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 181.10 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 74.49 pm. For H + HF reaction, the approximate position of the transition state is where r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = 74.49 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = 181.10 pm. In both situations, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
This is determined by finding the distance when force equals or closes to zero. As F is a bigger atom, the distance between F and H are expected to be bigger.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot3bl1718.png |500 px|thumb|center|Figure 13: Trajectory for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at transition state]]&lt;br /&gt;
[[File:Surface_Plot4bl1718.png |500 px|thumb|center|Figure 14: Trajectory for H + HF reaction at transition state]]&lt;br /&gt;
&lt;br /&gt;
==== Report the activation energy for both reactions ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy at saddle point - energy of reactants.The energy of reactants is determined as the minimum energy by changing r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; while keeping r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; large. For F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the energy of reactants is -435.100 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy is 1.12 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.  For H + HF reaction, the energy at transition state is -433.981 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the energy of reactants is -560.600 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.Thus, the activation energy for H + HF reaction is 126.6 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_8.png |500 px|thumb|center|Figure 15: Reactant energy in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_9.png |500 px|thumb|center|Figure 16: reactant energy in H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
=== Reaction dynamics ===&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally ====&lt;br /&gt;
&lt;br /&gt;
The condition of reaction trajectory is set as the same r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; as its saddle point but a smaller r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;, both momenta are set at zero (i.e. zero initial kinetic energy). From the Animation, the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule approaches F atom as it vibrates. At a point, the closer H atom is attracted by F and the formed HF molecule starts to vibrate. The rest H atom gains kinetic energy and repulse from the HF molecule. Since the initial kinetic energy in the system is zero, the Animation shows that some vibrational energy is transferred into kinetic energy. This is also shown in Momenta vs Time plot (Figure 17). The increase in amplitude suggests that a gain in kinetic energy. According to the reference, the reaction is occurred on a highly repulsive surface. When the bimolecule approaches F, the repulsion between Hs causes the closer H atom to recoil, pushing the H atom to F and AB vibration is produced.A schematic representation is also shown in the reference. (Figure 18) &amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the release of energy can be measured by a thermometer. However, it may be hard to measure as the reaction is carried out in gas phase. A more accurate way is to use a bomb calorimetry. The reaction takes place in a sealed container in water. Heat from reaction in the sealed metal container flow to the water. The temperature difference of water can be measured and the heat flow can be determined.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation14bl1718.png |500 px|thumb|center|Figure 17: Momenta vs Time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
[[File:bl1718_11.png |500 px|thumb|center|Figure 18: Schematic representation of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 181.10 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 74.49 pm, so the initial potential energy is the same as its transition state.By increasing the momenta, the kinetic energy of biomolecule increases.From the Contour plots, some curves show the presence of barrier recrossing. This suggests that in translation mode, most released energy is gone to vibration energy causing the increase possibility of barrier recrossing. Whereas in vibration mode, most released energy is gone to translation energy, so the repulsed H atom has more kinetic energy. The  distribution of energy in two difference modes affect the efficiency of reaction. Vibration mode is more efficient than translation mode.&lt;br /&gt;
The position of transition state in F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction suggests its surface being a Type-I barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_13.png |500 px|thumb|center|Figure 19: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
[[File:bl1718_12.png |500 px|thumb|center|Figure 20: Contour plots of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction with increasing p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Observation of changing initial conditions in H + HF reaction&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is set at 92 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is set at 220 pm.With an increase in p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, the trajectory curve to the product region. This shows with enough translation energy, the reaction can occur. In this system, vibration mode is also more efficient than translation mode. As a reverse of the previous reaction, it is considered to have a late-barrier surface.&amp;lt;ref name=&amp;quot;Chemical Kinetics&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name = &amp;quot;Chemical Kinetics&amp;quot;&amp;gt;Chapter 12.3,K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bl1718_14.png |500 px|thumb|center|Figure 21: Contour plots of H + HF reaction with increasing p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;]]&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:xs2218&amp;diff=812733</id>
		<title>MRD:xs2218</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:xs2218&amp;diff=812733"/>
		<updated>2020-06-04T12:37:52Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Part 5: Different modes of distribution of energy */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Molecular Reaction Dynamic Lab==&lt;br /&gt;
===Exercise1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system===&lt;br /&gt;
&lt;br /&gt;
====Part 1: Definition of transition state====&lt;br /&gt;
On a potential energy surface diagram, the transition state is mathematically defined as a first-order saddle point, ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0. &lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.  To distinguish from the local minimum on the PES, the first-order saddle point is at a minimum in all directions except for one and the trajectories near the transition state roll towards reactants or products. See the surface plot below, the TS is at a saddle point.&lt;br /&gt;
[[File:Q1_xs2218.png|thumb|center|Surface plot of transition state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, you could have included a description of the second derivative and what this tells us about the maxima and minima directions? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 2: Transition state approximation====&lt;br /&gt;
My best estimate of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;is 90.775pm, it is when the force along AB and BC is 0 KJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The atoms are not bonded at TS&lt;br /&gt;
The internuclear distance vs time plot shows 2 straight lines illustrating that when the atoms are at the transition state, the internuclear distance does not change, no such oscillating behavior where the 2 lines are wavy when not at TS.&lt;br /&gt;
[[File:Exe1 Q2.png|thumb|center|internuclear distance vs time plot at TS|350px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Okk, ensure that you refer to the figures numerically in the text and they are labelled as such i.e. Figure 1 shows X.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 3: Difference between MEP and Dynamics calculation type ====&lt;br /&gt;
As shown from the surface plots below, two different calculation types give different trajectories. The MEP shows the minimal energy path that any point on the path is at energy minimum in all directions perpendicular to the path which passes through at least one saddle point.  Looking at the plots from the same angle, the dynamic surface plot gives a wavy line coming out of the BC distance axis whereas the MEP surface plot gives a relatively straight line within the BC distance axis.&lt;br /&gt;
[[File:Exe1_Q3_mep_xs2218.png|thumb|left|Surface plot of MEP calculation type.|350px]]&lt;br /&gt;
[[File:Exe1_Q3_dynamics_xs2218.png|thumb|center|Surface plot of dynamics calculation type.|350px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Whilst this comparison is correct, you have not attributed what the wavy or straight lines correspond to. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 4: Reactive and unreactive trajectories====&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Table 1 r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74pm, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=200pm&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.280 || yes || AB are bonded at first until B bonds with C and A moves away, prodct BC formed || [[File:table1_row1.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1 || -420.077 || No || AB is always bonded, no product formed || [[File:table1_row2.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.977 || yes || AB are bonded at first until B is bonded with C and A moves away, prodct BC formed || [[File:table1_row3.png|150px]] || &lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.277 || No || AB are bonded at first until B bonds with C, but eventually B is back to bonded with A, C moves away, no product BC formed || [[File:table1_row4.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.477 || yes || AB are bonded at first until C approaches and B bonds with C, then B bonds with A again, eventually, B bonds with C and forms a product BC, A moves away|| [[File:table1_row5.png|150px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
In conclusion, trajectories starting with the same positions but with higher values of momenta would not always be reactive, although the total energy is getting more positive, therefore, the hypothesis is not supported&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|The descriptions for the table could do with a little more detail. In the last two trajectories we can see some clearly interesting behaviour with the barrier recrossing.Your conclusion is correct but could do with a little more detail as it is a bit unclear. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 5: Transition State Theory====&lt;br /&gt;
The Transition State Theory assumes that R&amp;lt;sub&amp;gt;cl&amp;lt;/sub&amp;gt; is that all trajectories with a KE greater than the activation energy will be reactive, however, our experimental has suggested that this is not true.&lt;br /&gt;
Transition state theory is based on classical mechanics, Quasi-equilibrium basically covers that if the atoms did not have enough energy to collide to form the TS, the reaction would not be feasible. However, in quantum mechanics, as long as the barrier has a finite amount of energy, the atoms can still tunnel across the barrier which means that the reaction could still be feasible even if the atoms do not collide enough energy to cross the energy barrier. &lt;br /&gt;
Quantum tunneling is minimal in TS theory, if quantum tunneling was present, the reaction rate would increase. &lt;br /&gt;
In transition state theory, it assumes that the step from TS to products is the rate-determining step, but  in reality, it might not be true, the reaction rate would. be decreased&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Make it clear which aspect of the table you are referring to. Quasi equilibrum refers to the concentration of TS remaming in relation to the concentration of reactant - i.e. the TS is treated as in chemical equilibria with the reactant. Barrier recrossing is not permitted in TST - is this observed in the above table? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===Exercise2: F-H-H system===&lt;br /&gt;
&lt;br /&gt;
====Part 1: PES inspection====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic, whereas HF + H is endothermic.&lt;br /&gt;
&lt;br /&gt;
H-H bond strength is weaker than the H-F bond. The energy absorbed to break the F-F bond is smaller than the energy needed to make the new bond H-F, the excess energy is then released as heat, so the reaction is exothermic. However, for HF + H, more energy is needed to break the H-F bond than to make the F-F bond, overall, energy is being absorbed rather than released, so the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok good answer just make it clear you are referring to the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 2: Transition State Approximation====&lt;br /&gt;
The approximate position of transition state:  r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=181.1 pm, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=74.488pm&lt;br /&gt;
The forces along AB and BC at this position are both 0. According to Hammond Postulate, an  exothermic reaction has an early TS, whereas an endothermic reaction has a late TS, therefore, one of the eigenvalues at TS is positive, another one is negative. In this case, the Hessian eigenvalues are -0.002 and +0.332.&lt;br /&gt;
As shown in the surface plot below, now it is at a saddle point which confirms the atoms are at the transition state.&lt;br /&gt;
[[File:Q7_xs2218_new.png|thumb|center|Surface Plot of transition state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok succinct answer. Hammond postulte could do with a reference. The Hessian value for BC indicates deviation from the actual TS. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 3: Activation Energy====&lt;br /&gt;
The transition state energy is reported as -433.981 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
A plot of energy vs time is plotted at TS as shown below.&lt;br /&gt;
[[File:Exe2_Q3_TSenergy.png|thumb|center|Energy vs Time plot at TS for F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
For the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the initial state energy is -435.059 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Activation energy can then be calculated as 1.08 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
[[File:Exe2_Q3_exoenergy.png|thumb|center|Energy vs Time plot at initial state for exothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
For the endothermic reaction HF + H, the initial state energy is -560.700 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Activation energy for this reaction is 126.02 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
[[File:Exe2_Q3_endoenergy.png|thumb|center|Energy vs Time plot at initial state for endothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
By locating a structure neighboring the TS, the plot of Energy vs time shows that the energy dropping clearly.&lt;br /&gt;
[[File:Exe2_Q3_endoenergy_new.png|thumb|center|Energy vs Time plot at the neighboring structure of  transition state for endothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
(The plot of the neighboring structure of TS for exothermic reaction is not shown because the difference is too small to be spotted.)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great answer! Make sure to refer to the figures in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 4: Release of reaction energy====&lt;br /&gt;
The release of reaction energy is basically a release of vibrational kinetic energy converted from potential energy. A contour plot of a reactive trajectory is shown below to illustrate.&lt;br /&gt;
[[File:Exe2_Q4_xs2218.png|thumb|center|A contour plot of a reactive trajectory in a F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
An experimental method to confirm it is IR spectrometry. IR absorption would have stronger overtones that measuring the transition from the first to second state, while IR emission measures the transition from the first to the ground state.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Slighlty confusing answer, a refernece may have helped. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 5: Different modes of distribution of energy====&lt;br /&gt;
In general, vibrational energy is better than promoting endothermic reactions than exothermic reactions, whereas translational energy is better than promoting exothermic reactions than endothermic reactions.&lt;br /&gt;
When having translational energy, the atoms would bounce onto the potential wall and bounce back. When having vibrational energy, the atoms fall down the reaction channel and overcome the reaction barrier, forming the product.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Make sure to set up your argument in reference to literature - i.e. here the first sentence refers to Polanyis rules. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Plot 1 and 2 illustrate the situation when a huge amount of energy is put into the system on the H-H vibration, the trajectory moves from the left-hand side of the plot to the right-hand side.&lt;br /&gt;
[[File:Exe2_Q5_1.png|thumb|left|Plot 1: when the H-H vibration at low energy in an F-H-H system.]]&lt;br /&gt;
[[File:Exe2_Q5_2.png|thumb|center|Plot 2: when the H-H vibration at high energy in an F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|The results need to be expressed in terms of reactivity or unreactivity depending on the dependence on vibrational or translational energy. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
When the momentum of F-H is increased slightly, the energy of the overall system is reduced by reducing the momentum of H-H which means the H-H vibrational energy is reduced, the trajectory plot below looks similar to plot 2 when there is high vibrational energy on H-H but with slightly lower F-H momentum. It further confirms that the exothermic reaction is promoted by translational energy better.&lt;br /&gt;
[[File:Exe2_Q5_3.png|thumb|center|Plot 3: when F-H momentum is  slightly increased and H-H momentum is reduced an F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Waht about the vibrational energy ? Could you have confirmed this the other way round? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===References===&lt;br /&gt;
1. R. J. Silbey, R. A. Alberty, M. G. Bawendi Physical Chemistry, 4th ed, John Wiley &amp;amp; Sons, 2005.&lt;br /&gt;
&lt;br /&gt;
2. J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998, chapter 10&lt;br /&gt;
&lt;br /&gt;
3. K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987, chapter 4&lt;br /&gt;
&lt;br /&gt;
4. M. J. Pilling, P. W. Seakins Reaction Kinetics, 2nd ed., OUP, 1995, chapter 4&lt;br /&gt;
&lt;br /&gt;
5.Atkins, de Paula, Keeler, Physical Chemistry, 11th ed&lt;br /&gt;
&lt;br /&gt;
6. I. N. Levine, Physical Chemistry, McGraw-Hill, 4th ed&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok it is good you have included these, make sure it is clear in the text where each reference refers to. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:xs2218&amp;diff=812732</id>
		<title>MRD:xs2218</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:xs2218&amp;diff=812732"/>
		<updated>2020-06-04T12:36:21Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Molecular Reaction Dynamic Lab==&lt;br /&gt;
===Exercise1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system===&lt;br /&gt;
&lt;br /&gt;
====Part 1: Definition of transition state====&lt;br /&gt;
On a potential energy surface diagram, the transition state is mathematically defined as a first-order saddle point, ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0. &lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.  To distinguish from the local minimum on the PES, the first-order saddle point is at a minimum in all directions except for one and the trajectories near the transition state roll towards reactants or products. See the surface plot below, the TS is at a saddle point.&lt;br /&gt;
[[File:Q1_xs2218.png|thumb|center|Surface plot of transition state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, you could have included a description of the second derivative and what this tells us about the maxima and minima directions? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 2: Transition state approximation====&lt;br /&gt;
My best estimate of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;is 90.775pm, it is when the force along AB and BC is 0 KJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The atoms are not bonded at TS&lt;br /&gt;
The internuclear distance vs time plot shows 2 straight lines illustrating that when the atoms are at the transition state, the internuclear distance does not change, no such oscillating behavior where the 2 lines are wavy when not at TS.&lt;br /&gt;
[[File:Exe1 Q2.png|thumb|center|internuclear distance vs time plot at TS|350px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Okk, ensure that you refer to the figures numerically in the text and they are labelled as such i.e. Figure 1 shows X.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 3: Difference between MEP and Dynamics calculation type ====&lt;br /&gt;
As shown from the surface plots below, two different calculation types give different trajectories. The MEP shows the minimal energy path that any point on the path is at energy minimum in all directions perpendicular to the path which passes through at least one saddle point.  Looking at the plots from the same angle, the dynamic surface plot gives a wavy line coming out of the BC distance axis whereas the MEP surface plot gives a relatively straight line within the BC distance axis.&lt;br /&gt;
[[File:Exe1_Q3_mep_xs2218.png|thumb|left|Surface plot of MEP calculation type.|350px]]&lt;br /&gt;
[[File:Exe1_Q3_dynamics_xs2218.png|thumb|center|Surface plot of dynamics calculation type.|350px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Whilst this comparison is correct, you have not attributed what the wavy or straight lines correspond to. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 4: Reactive and unreactive trajectories====&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Table 1 r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74pm, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=200pm&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.280 || yes || AB are bonded at first until B bonds with C and A moves away, prodct BC formed || [[File:table1_row1.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1 || -420.077 || No || AB is always bonded, no product formed || [[File:table1_row2.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.977 || yes || AB are bonded at first until B is bonded with C and A moves away, prodct BC formed || [[File:table1_row3.png|150px]] || &lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.277 || No || AB are bonded at first until B bonds with C, but eventually B is back to bonded with A, C moves away, no product BC formed || [[File:table1_row4.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.477 || yes || AB are bonded at first until C approaches and B bonds with C, then B bonds with A again, eventually, B bonds with C and forms a product BC, A moves away|| [[File:table1_row5.png|150px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
In conclusion, trajectories starting with the same positions but with higher values of momenta would not always be reactive, although the total energy is getting more positive, therefore, the hypothesis is not supported&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|The descriptions for the table could do with a little more detail. In the last two trajectories we can see some clearly interesting behaviour with the barrier recrossing.Your conclusion is correct but could do with a little more detail as it is a bit unclear. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 5: Transition State Theory====&lt;br /&gt;
The Transition State Theory assumes that R&amp;lt;sub&amp;gt;cl&amp;lt;/sub&amp;gt; is that all trajectories with a KE greater than the activation energy will be reactive, however, our experimental has suggested that this is not true.&lt;br /&gt;
Transition state theory is based on classical mechanics, Quasi-equilibrium basically covers that if the atoms did not have enough energy to collide to form the TS, the reaction would not be feasible. However, in quantum mechanics, as long as the barrier has a finite amount of energy, the atoms can still tunnel across the barrier which means that the reaction could still be feasible even if the atoms do not collide enough energy to cross the energy barrier. &lt;br /&gt;
Quantum tunneling is minimal in TS theory, if quantum tunneling was present, the reaction rate would increase. &lt;br /&gt;
In transition state theory, it assumes that the step from TS to products is the rate-determining step, but  in reality, it might not be true, the reaction rate would. be decreased&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Make it clear which aspect of the table you are referring to. Quasi equilibrum refers to the concentration of TS remaming in relation to the concentration of reactant - i.e. the TS is treated as in chemical equilibria with the reactant. Barrier recrossing is not permitted in TST - is this observed in the above table? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===Exercise2: F-H-H system===&lt;br /&gt;
&lt;br /&gt;
====Part 1: PES inspection====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic, whereas HF + H is endothermic.&lt;br /&gt;
&lt;br /&gt;
H-H bond strength is weaker than the H-F bond. The energy absorbed to break the F-F bond is smaller than the energy needed to make the new bond H-F, the excess energy is then released as heat, so the reaction is exothermic. However, for HF + H, more energy is needed to break the H-F bond than to make the F-F bond, overall, energy is being absorbed rather than released, so the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok good answer just make it clear you are referring to the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 2: Transition State Approximation====&lt;br /&gt;
The approximate position of transition state:  r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=181.1 pm, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=74.488pm&lt;br /&gt;
The forces along AB and BC at this position are both 0. According to Hammond Postulate, an  exothermic reaction has an early TS, whereas an endothermic reaction has a late TS, therefore, one of the eigenvalues at TS is positive, another one is negative. In this case, the Hessian eigenvalues are -0.002 and +0.332.&lt;br /&gt;
As shown in the surface plot below, now it is at a saddle point which confirms the atoms are at the transition state.&lt;br /&gt;
[[File:Q7_xs2218_new.png|thumb|center|Surface Plot of transition state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok succinct answer. Hammond postulte could do with a reference. The Hessian value for BC indicates deviation from the actual TS. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 3: Activation Energy====&lt;br /&gt;
The transition state energy is reported as -433.981 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
A plot of energy vs time is plotted at TS as shown below.&lt;br /&gt;
[[File:Exe2_Q3_TSenergy.png|thumb|center|Energy vs Time plot at TS for F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
For the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the initial state energy is -435.059 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Activation energy can then be calculated as 1.08 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
[[File:Exe2_Q3_exoenergy.png|thumb|center|Energy vs Time plot at initial state for exothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
For the endothermic reaction HF + H, the initial state energy is -560.700 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Activation energy for this reaction is 126.02 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
[[File:Exe2_Q3_endoenergy.png|thumb|center|Energy vs Time plot at initial state for endothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
By locating a structure neighboring the TS, the plot of Energy vs time shows that the energy dropping clearly.&lt;br /&gt;
[[File:Exe2_Q3_endoenergy_new.png|thumb|center|Energy vs Time plot at the neighboring structure of  transition state for endothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
(The plot of the neighboring structure of TS for exothermic reaction is not shown because the difference is too small to be spotted.)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great answer! Make sure to refer to the figures in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 4: Release of reaction energy====&lt;br /&gt;
The release of reaction energy is basically a release of vibrational kinetic energy converted from potential energy. A contour plot of a reactive trajectory is shown below to illustrate.&lt;br /&gt;
[[File:Exe2_Q4_xs2218.png|thumb|center|A contour plot of a reactive trajectory in a F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
An experimental method to confirm it is IR spectrometry. IR absorption would have stronger overtones that measuring the transition from the first to second state, while IR emission measures the transition from the first to the ground state.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Slighlty confusing answer, a refernece may have helped. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 5: Different modes of distribution of energy====&lt;br /&gt;
In general, vibrational energy is better than promoting endothermic reactions than exothermic reactions, whereas translational energy is better than promoting exothermic reactions than endothermic reactions.&lt;br /&gt;
When having translational energy, the atoms would bounce onto the potential wall and bounce back. When having vibrational energy, the atoms fall down the reaction channel and overcome the reaction barrier, forming the product.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Make sure to set up your argument in reference to literature - i.e. here the first sentence refers to Polanyis rules. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Plot 1 and 2 illustrate the situation when a huge amount of energy is put into the system on the H-H vibration, the trajectory moves from the left-hand side of the plot to the right-hand side.&lt;br /&gt;
[[File:Exe2_Q5_1.png|thumb|left|Plot 1: when the H-H vibration at low energy in an F-H-H system.]]&lt;br /&gt;
[[File:Exe2_Q5_2.png|thumb|center|Plot 2: when the H-H vibration at high energy in an F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When the momentum of F-H is increased slightly, the energy of the overall system is reduced by reducing the momentum of H-H which means the H-H vibrational energy is reduced, the trajectory plot below looks similar to plot 2 when there is high vibrational energy on H-H but with slightly lower F-H momentum. It further confirms that the exothermic reaction is promoted by translational energy better.&lt;br /&gt;
[[File:Exe2_Q5_3.png|thumb|center|Plot 3: when F-H momentum is  slightly increased and H-H momentum is reduced an F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Waht about the vibrational energy ? Could you have confirmed this the other way round? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===References===&lt;br /&gt;
1. R. J. Silbey, R. A. Alberty, M. G. Bawendi Physical Chemistry, 4th ed, John Wiley &amp;amp; Sons, 2005.&lt;br /&gt;
&lt;br /&gt;
2. J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998, chapter 10&lt;br /&gt;
&lt;br /&gt;
3. K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987, chapter 4&lt;br /&gt;
&lt;br /&gt;
4. M. J. Pilling, P. W. Seakins Reaction Kinetics, 2nd ed., OUP, 1995, chapter 4&lt;br /&gt;
&lt;br /&gt;
5.Atkins, de Paula, Keeler, Physical Chemistry, 11th ed&lt;br /&gt;
&lt;br /&gt;
6. I. N. Levine, Physical Chemistry, McGraw-Hill, 4th ed&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok it is good you have included these, make sure it is clear in the text where each reference refers to. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:xs2218&amp;diff=812731</id>
		<title>MRD:xs2218</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:xs2218&amp;diff=812731"/>
		<updated>2020-06-04T12:35:55Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Part 5: Different modes of distribution of energy */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Molecular Reaction Dynamic Lab==&lt;br /&gt;
===Exercise1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system===&lt;br /&gt;
&lt;br /&gt;
====Part 1: Definition of transition state====&lt;br /&gt;
On a potential energy surface diagram, the transition state is mathematically defined as a first-order saddle point, ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0. &lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.  To distinguish from the local minimum on the PES, the first-order saddle point is at a minimum in all directions except for one and the trajectories near the transition state roll towards reactants or products. See the surface plot below, the TS is at a saddle point.&lt;br /&gt;
[[File:Q1_xs2218.png|thumb|center|Surface plot of transition state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, you could have included a description of the second derivative and what this tells us about the maxima and minima directions? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 2: Transition state approximation====&lt;br /&gt;
My best estimate of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;is 90.775pm, it is when the force along AB and BC is 0 KJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The atoms are not bonded at TS&lt;br /&gt;
The internuclear distance vs time plot shows 2 straight lines illustrating that when the atoms are at the transition state, the internuclear distance does not change, no such oscillating behavior where the 2 lines are wavy when not at TS.&lt;br /&gt;
[[File:Exe1 Q2.png|thumb|center|internuclear distance vs time plot at TS|350px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Okk, ensure that you refer to the figures numerically in the text and they are labelled as such i.e. Figure 1 shows X.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 3: Difference between MEP and Dynamics calculation type ====&lt;br /&gt;
As shown from the surface plots below, two different calculation types give different trajectories. The MEP shows the minimal energy path that any point on the path is at energy minimum in all directions perpendicular to the path which passes through at least one saddle point.  Looking at the plots from the same angle, the dynamic surface plot gives a wavy line coming out of the BC distance axis whereas the MEP surface plot gives a relatively straight line within the BC distance axis.&lt;br /&gt;
[[File:Exe1_Q3_mep_xs2218.png|thumb|left|Surface plot of MEP calculation type.|350px]]&lt;br /&gt;
[[File:Exe1_Q3_dynamics_xs2218.png|thumb|center|Surface plot of dynamics calculation type.|350px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Whilst this comparison is correct, you have not attributed what the wavy or straight lines correspond to. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 4: Reactive and unreactive trajectories====&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Table 1 r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74pm, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=200pm&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.280 || yes || AB are bonded at first until B bonds with C and A moves away, prodct BC formed || [[File:table1_row1.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1 || -420.077 || No || AB is always bonded, no product formed || [[File:table1_row2.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.977 || yes || AB are bonded at first until B is bonded with C and A moves away, prodct BC formed || [[File:table1_row3.png|150px]] || &lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.277 || No || AB are bonded at first until B bonds with C, but eventually B is back to bonded with A, C moves away, no product BC formed || [[File:table1_row4.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.477 || yes || AB are bonded at first until C approaches and B bonds with C, then B bonds with A again, eventually, B bonds with C and forms a product BC, A moves away|| [[File:table1_row5.png|150px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
In conclusion, trajectories starting with the same positions but with higher values of momenta would not always be reactive, although the total energy is getting more positive, therefore, the hypothesis is not supported&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|The descriptions for the table could do with a little more detail. In the last two trajectories we can see some clearly interesting behaviour with the barrier recrossing.Your conclusion is correct but could do with a little more detail as it is a bit unclear. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 5: Transition State Theory====&lt;br /&gt;
The Transition State Theory assumes that R&amp;lt;sub&amp;gt;cl&amp;lt;/sub&amp;gt; is that all trajectories with a KE greater than the activation energy will be reactive, however, our experimental has suggested that this is not true.&lt;br /&gt;
Transition state theory is based on classical mechanics, Quasi-equilibrium basically covers that if the atoms did not have enough energy to collide to form the TS, the reaction would not be feasible. However, in quantum mechanics, as long as the barrier has a finite amount of energy, the atoms can still tunnel across the barrier which means that the reaction could still be feasible even if the atoms do not collide enough energy to cross the energy barrier. &lt;br /&gt;
Quantum tunneling is minimal in TS theory, if quantum tunneling was present, the reaction rate would increase. &lt;br /&gt;
In transition state theory, it assumes that the step from TS to products is the rate-determining step, but  in reality, it might not be true, the reaction rate would. be decreased&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Make it clear which aspect of the table you are referring to. Quasi equilibrum refers to the concentration of TS remaming in relation to the concentration of reactant - i.e. the TS is treated as in chemical equilibria with the reactant. Barrier recrossing is not permitted in TST - is this observed in the above table? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===Exercise2: F-H-H system===&lt;br /&gt;
&lt;br /&gt;
====Part 1: PES inspection====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic, whereas HF + H is endothermic.&lt;br /&gt;
&lt;br /&gt;
H-H bond strength is weaker than the H-F bond. The energy absorbed to break the F-F bond is smaller than the energy needed to make the new bond H-F, the excess energy is then released as heat, so the reaction is exothermic. However, for HF + H, more energy is needed to break the H-F bond than to make the F-F bond, overall, energy is being absorbed rather than released, so the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok good answer just make it clear you are referring to the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 2: Transition State Approximation====&lt;br /&gt;
The approximate position of transition state:  r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=181.1 pm, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=74.488pm&lt;br /&gt;
The forces along AB and BC at this position are both 0. According to Hammond Postulate, an  exothermic reaction has an early TS, whereas an endothermic reaction has a late TS, therefore, one of the eigenvalues at TS is positive, another one is negative. In this case, the Hessian eigenvalues are -0.002 and +0.332.&lt;br /&gt;
As shown in the surface plot below, now it is at a saddle point which confirms the atoms are at the transition state.&lt;br /&gt;
[[File:Q7_xs2218_new.png|thumb|center|Surface Plot of transition state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok succinct answer. Hammond postulte could do with a reference. The Hessian value for BC indicates deviation from the actual TS. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 3: Activation Energy====&lt;br /&gt;
The transition state energy is reported as -433.981 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
A plot of energy vs time is plotted at TS as shown below.&lt;br /&gt;
[[File:Exe2_Q3_TSenergy.png|thumb|center|Energy vs Time plot at TS for F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
For the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the initial state energy is -435.059 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Activation energy can then be calculated as 1.08 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
[[File:Exe2_Q3_exoenergy.png|thumb|center|Energy vs Time plot at initial state for exothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
For the endothermic reaction HF + H, the initial state energy is -560.700 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Activation energy for this reaction is 126.02 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
[[File:Exe2_Q3_endoenergy.png|thumb|center|Energy vs Time plot at initial state for endothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
By locating a structure neighboring the TS, the plot of Energy vs time shows that the energy dropping clearly.&lt;br /&gt;
[[File:Exe2_Q3_endoenergy_new.png|thumb|center|Energy vs Time plot at the neighboring structure of  transition state for endothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
(The plot of the neighboring structure of TS for exothermic reaction is not shown because the difference is too small to be spotted.)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great answer! Make sure to refer to the figures in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 4: Release of reaction energy====&lt;br /&gt;
The release of reaction energy is basically a release of vibrational kinetic energy converted from potential energy. A contour plot of a reactive trajectory is shown below to illustrate.&lt;br /&gt;
[[File:Exe2_Q4_xs2218.png|thumb|center|A contour plot of a reactive trajectory in a F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
An experimental method to confirm it is IR spectrometry. IR absorption would have stronger overtones that measuring the transition from the first to second state, while IR emission measures the transition from the first to the ground state.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Slighlty confusing answer, a refernece may have helped. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 5: Different modes of distribution of energy====&lt;br /&gt;
In general, vibrational energy is better than promoting endothermic reactions than exothermic reactions, whereas translational energy is better than promoting exothermic reactions than endothermic reactions.&lt;br /&gt;
When having translational energy, the atoms would bounce onto the potential wall and bounce back. When having vibrational energy, the atoms fall down the reaction channel and overcome the reaction barrier, forming the product.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green| Make sure to set up your argument in reference to literature - i.e. here the first sentence refers to Polanyis rules. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Plot 1 and 2 illustrate the situation when a huge amount of energy is put into the system on the H-H vibration, the trajectory moves from the left-hand side of the plot to the right-hand side.&lt;br /&gt;
[[File:Exe2_Q5_1.png|thumb|left|Plot 1: when the H-H vibration at low energy in an F-H-H system.]]&lt;br /&gt;
[[File:Exe2_Q5_2.png|thumb|center|Plot 2: when the H-H vibration at high energy in an F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When the momentum of F-H is increased slightly, the energy of the overall system is reduced by reducing the momentum of H-H which means the H-H vibrational energy is reduced, the trajectory plot below looks similar to plot 2 when there is high vibrational energy on H-H but with slightly lower F-H momentum. It further confirms that the exothermic reaction is promoted by translational energy better.&lt;br /&gt;
[[File:Exe2_Q5_3.png|thumb|center|Plot 3: when F-H momentum is  slightly increased and H-H momentum is reduced an F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Waht about the vibrational energy ? Could you have confirmed this the other way round? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===References===&lt;br /&gt;
1. R. J. Silbey, R. A. Alberty, M. G. Bawendi Physical Chemistry, 4th ed, John Wiley &amp;amp; Sons, 2005.&lt;br /&gt;
&lt;br /&gt;
2. J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998, chapter 10&lt;br /&gt;
&lt;br /&gt;
3. K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987, chapter 4&lt;br /&gt;
&lt;br /&gt;
4. M. J. Pilling, P. W. Seakins Reaction Kinetics, 2nd ed., OUP, 1995, chapter 4&lt;br /&gt;
&lt;br /&gt;
5.Atkins, de Paula, Keeler, Physical Chemistry, 11th ed&lt;br /&gt;
&lt;br /&gt;
6. I. N. Levine, Physical Chemistry, McGraw-Hill, 4th ed&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:xs2218&amp;diff=812730</id>
		<title>MRD:xs2218</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:xs2218&amp;diff=812730"/>
		<updated>2020-06-04T12:34:15Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Part 4: Release of reaction energy */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Molecular Reaction Dynamic Lab==&lt;br /&gt;
===Exercise1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system===&lt;br /&gt;
&lt;br /&gt;
====Part 1: Definition of transition state====&lt;br /&gt;
On a potential energy surface diagram, the transition state is mathematically defined as a first-order saddle point, ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0. &lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.  To distinguish from the local minimum on the PES, the first-order saddle point is at a minimum in all directions except for one and the trajectories near the transition state roll towards reactants or products. See the surface plot below, the TS is at a saddle point.&lt;br /&gt;
[[File:Q1_xs2218.png|thumb|center|Surface plot of transition state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, you could have included a description of the second derivative and what this tells us about the maxima and minima directions? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 2: Transition state approximation====&lt;br /&gt;
My best estimate of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;is 90.775pm, it is when the force along AB and BC is 0 KJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The atoms are not bonded at TS&lt;br /&gt;
The internuclear distance vs time plot shows 2 straight lines illustrating that when the atoms are at the transition state, the internuclear distance does not change, no such oscillating behavior where the 2 lines are wavy when not at TS.&lt;br /&gt;
[[File:Exe1 Q2.png|thumb|center|internuclear distance vs time plot at TS|350px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Okk, ensure that you refer to the figures numerically in the text and they are labelled as such i.e. Figure 1 shows X.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 3: Difference between MEP and Dynamics calculation type ====&lt;br /&gt;
As shown from the surface plots below, two different calculation types give different trajectories. The MEP shows the minimal energy path that any point on the path is at energy minimum in all directions perpendicular to the path which passes through at least one saddle point.  Looking at the plots from the same angle, the dynamic surface plot gives a wavy line coming out of the BC distance axis whereas the MEP surface plot gives a relatively straight line within the BC distance axis.&lt;br /&gt;
[[File:Exe1_Q3_mep_xs2218.png|thumb|left|Surface plot of MEP calculation type.|350px]]&lt;br /&gt;
[[File:Exe1_Q3_dynamics_xs2218.png|thumb|center|Surface plot of dynamics calculation type.|350px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Whilst this comparison is correct, you have not attributed what the wavy or straight lines correspond to. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 4: Reactive and unreactive trajectories====&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Table 1 r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74pm, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=200pm&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.280 || yes || AB are bonded at first until B bonds with C and A moves away, prodct BC formed || [[File:table1_row1.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1 || -420.077 || No || AB is always bonded, no product formed || [[File:table1_row2.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.977 || yes || AB are bonded at first until B is bonded with C and A moves away, prodct BC formed || [[File:table1_row3.png|150px]] || &lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.277 || No || AB are bonded at first until B bonds with C, but eventually B is back to bonded with A, C moves away, no product BC formed || [[File:table1_row4.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.477 || yes || AB are bonded at first until C approaches and B bonds with C, then B bonds with A again, eventually, B bonds with C and forms a product BC, A moves away|| [[File:table1_row5.png|150px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
In conclusion, trajectories starting with the same positions but with higher values of momenta would not always be reactive, although the total energy is getting more positive, therefore, the hypothesis is not supported&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|The descriptions for the table could do with a little more detail. In the last two trajectories we can see some clearly interesting behaviour with the barrier recrossing.Your conclusion is correct but could do with a little more detail as it is a bit unclear. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 5: Transition State Theory====&lt;br /&gt;
The Transition State Theory assumes that R&amp;lt;sub&amp;gt;cl&amp;lt;/sub&amp;gt; is that all trajectories with a KE greater than the activation energy will be reactive, however, our experimental has suggested that this is not true.&lt;br /&gt;
Transition state theory is based on classical mechanics, Quasi-equilibrium basically covers that if the atoms did not have enough energy to collide to form the TS, the reaction would not be feasible. However, in quantum mechanics, as long as the barrier has a finite amount of energy, the atoms can still tunnel across the barrier which means that the reaction could still be feasible even if the atoms do not collide enough energy to cross the energy barrier. &lt;br /&gt;
Quantum tunneling is minimal in TS theory, if quantum tunneling was present, the reaction rate would increase. &lt;br /&gt;
In transition state theory, it assumes that the step from TS to products is the rate-determining step, but  in reality, it might not be true, the reaction rate would. be decreased&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Make it clear which aspect of the table you are referring to. Quasi equilibrum refers to the concentration of TS remaming in relation to the concentration of reactant - i.e. the TS is treated as in chemical equilibria with the reactant. Barrier recrossing is not permitted in TST - is this observed in the above table? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===Exercise2: F-H-H system===&lt;br /&gt;
&lt;br /&gt;
====Part 1: PES inspection====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic, whereas HF + H is endothermic.&lt;br /&gt;
&lt;br /&gt;
H-H bond strength is weaker than the H-F bond. The energy absorbed to break the F-F bond is smaller than the energy needed to make the new bond H-F, the excess energy is then released as heat, so the reaction is exothermic. However, for HF + H, more energy is needed to break the H-F bond than to make the F-F bond, overall, energy is being absorbed rather than released, so the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok good answer just make it clear you are referring to the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 2: Transition State Approximation====&lt;br /&gt;
The approximate position of transition state:  r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=181.1 pm, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=74.488pm&lt;br /&gt;
The forces along AB and BC at this position are both 0. According to Hammond Postulate, an  exothermic reaction has an early TS, whereas an endothermic reaction has a late TS, therefore, one of the eigenvalues at TS is positive, another one is negative. In this case, the Hessian eigenvalues are -0.002 and +0.332.&lt;br /&gt;
As shown in the surface plot below, now it is at a saddle point which confirms the atoms are at the transition state.&lt;br /&gt;
[[File:Q7_xs2218_new.png|thumb|center|Surface Plot of transition state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok succinct answer. Hammond postulte could do with a reference. The Hessian value for BC indicates deviation from the actual TS. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 3: Activation Energy====&lt;br /&gt;
The transition state energy is reported as -433.981 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
A plot of energy vs time is plotted at TS as shown below.&lt;br /&gt;
[[File:Exe2_Q3_TSenergy.png|thumb|center|Energy vs Time plot at TS for F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
For the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the initial state energy is -435.059 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Activation energy can then be calculated as 1.08 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
[[File:Exe2_Q3_exoenergy.png|thumb|center|Energy vs Time plot at initial state for exothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
For the endothermic reaction HF + H, the initial state energy is -560.700 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Activation energy for this reaction is 126.02 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
[[File:Exe2_Q3_endoenergy.png|thumb|center|Energy vs Time plot at initial state for endothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
By locating a structure neighboring the TS, the plot of Energy vs time shows that the energy dropping clearly.&lt;br /&gt;
[[File:Exe2_Q3_endoenergy_new.png|thumb|center|Energy vs Time plot at the neighboring structure of  transition state for endothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
(The plot of the neighboring structure of TS for exothermic reaction is not shown because the difference is too small to be spotted.)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great answer! Make sure to refer to the figures in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 4: Release of reaction energy====&lt;br /&gt;
The release of reaction energy is basically a release of vibrational kinetic energy converted from potential energy. A contour plot of a reactive trajectory is shown below to illustrate.&lt;br /&gt;
[[File:Exe2_Q4_xs2218.png|thumb|center|A contour plot of a reactive trajectory in a F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
An experimental method to confirm it is IR spectrometry. IR absorption would have stronger overtones that measuring the transition from the first to second state, while IR emission measures the transition from the first to the ground state.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Slighlty confusing answer, a refernece may have helped. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 5: Different modes of distribution of energy====&lt;br /&gt;
In general, vibrational energy is better than promoting endothermic reactions than exothermic reactions, whereas translational energy is better than promoting exothermic reactions than endothermic reactions.&lt;br /&gt;
When having translational energy, the atoms would bounce onto the potential wall and bounce back. When having vibrational energy, the atoms fall down the reaction channel and overcome the reaction barrier, forming the product.&lt;br /&gt;
&lt;br /&gt;
Plot 1 and 2 illustrate the situation when a huge amount of energy is put into the system on the H-H vibration, the trajectory moves from the left-hand side of the plot to the right-hand side.&lt;br /&gt;
[[File:Exe2_Q5_1.png|thumb|left|Plot 1: when the H-H vibration at low energy in an F-H-H system.]]&lt;br /&gt;
[[File:Exe2_Q5_2.png|thumb|center|Plot 2: when the H-H vibration at high energy in an F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When the momentum of F-H is increased slightly, the energy of the overall system is reduced by reducing the momentum of H-H which means the H-H vibrational energy is reduced, the trajectory plot below looks similar to plot 2 when there is high vibrational energy on H-H but with slightly lower F-H momentum. It further confirms that the exothermic reaction is promoted by translational energy better.&lt;br /&gt;
[[File:Exe2_Q5_3.png|thumb|center|Plot 3: when F-H momentum is  slightly increased and H-H momentum is reduced an F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
===References===&lt;br /&gt;
1. R. J. Silbey, R. A. Alberty, M. G. Bawendi Physical Chemistry, 4th ed, John Wiley &amp;amp; Sons, 2005.&lt;br /&gt;
&lt;br /&gt;
2. J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998, chapter 10&lt;br /&gt;
&lt;br /&gt;
3. K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987, chapter 4&lt;br /&gt;
&lt;br /&gt;
4. M. J. Pilling, P. W. Seakins Reaction Kinetics, 2nd ed., OUP, 1995, chapter 4&lt;br /&gt;
&lt;br /&gt;
5.Atkins, de Paula, Keeler, Physical Chemistry, 11th ed&lt;br /&gt;
&lt;br /&gt;
6. I. N. Levine, Physical Chemistry, McGraw-Hill, 4th ed&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:xs2218&amp;diff=812729</id>
		<title>MRD:xs2218</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:xs2218&amp;diff=812729"/>
		<updated>2020-06-04T12:33:20Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Part 3: Activation Energy */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Molecular Reaction Dynamic Lab==&lt;br /&gt;
===Exercise1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system===&lt;br /&gt;
&lt;br /&gt;
====Part 1: Definition of transition state====&lt;br /&gt;
On a potential energy surface diagram, the transition state is mathematically defined as a first-order saddle point, ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0. &lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.  To distinguish from the local minimum on the PES, the first-order saddle point is at a minimum in all directions except for one and the trajectories near the transition state roll towards reactants or products. See the surface plot below, the TS is at a saddle point.&lt;br /&gt;
[[File:Q1_xs2218.png|thumb|center|Surface plot of transition state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, you could have included a description of the second derivative and what this tells us about the maxima and minima directions? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 2: Transition state approximation====&lt;br /&gt;
My best estimate of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;is 90.775pm, it is when the force along AB and BC is 0 KJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The atoms are not bonded at TS&lt;br /&gt;
The internuclear distance vs time plot shows 2 straight lines illustrating that when the atoms are at the transition state, the internuclear distance does not change, no such oscillating behavior where the 2 lines are wavy when not at TS.&lt;br /&gt;
[[File:Exe1 Q2.png|thumb|center|internuclear distance vs time plot at TS|350px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Okk, ensure that you refer to the figures numerically in the text and they are labelled as such i.e. Figure 1 shows X.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 3: Difference between MEP and Dynamics calculation type ====&lt;br /&gt;
As shown from the surface plots below, two different calculation types give different trajectories. The MEP shows the minimal energy path that any point on the path is at energy minimum in all directions perpendicular to the path which passes through at least one saddle point.  Looking at the plots from the same angle, the dynamic surface plot gives a wavy line coming out of the BC distance axis whereas the MEP surface plot gives a relatively straight line within the BC distance axis.&lt;br /&gt;
[[File:Exe1_Q3_mep_xs2218.png|thumb|left|Surface plot of MEP calculation type.|350px]]&lt;br /&gt;
[[File:Exe1_Q3_dynamics_xs2218.png|thumb|center|Surface plot of dynamics calculation type.|350px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Whilst this comparison is correct, you have not attributed what the wavy or straight lines correspond to. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 4: Reactive and unreactive trajectories====&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Table 1 r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74pm, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=200pm&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.280 || yes || AB are bonded at first until B bonds with C and A moves away, prodct BC formed || [[File:table1_row1.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1 || -420.077 || No || AB is always bonded, no product formed || [[File:table1_row2.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.977 || yes || AB are bonded at first until B is bonded with C and A moves away, prodct BC formed || [[File:table1_row3.png|150px]] || &lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.277 || No || AB are bonded at first until B bonds with C, but eventually B is back to bonded with A, C moves away, no product BC formed || [[File:table1_row4.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.477 || yes || AB are bonded at first until C approaches and B bonds with C, then B bonds with A again, eventually, B bonds with C and forms a product BC, A moves away|| [[File:table1_row5.png|150px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
In conclusion, trajectories starting with the same positions but with higher values of momenta would not always be reactive, although the total energy is getting more positive, therefore, the hypothesis is not supported&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|The descriptions for the table could do with a little more detail. In the last two trajectories we can see some clearly interesting behaviour with the barrier recrossing.Your conclusion is correct but could do with a little more detail as it is a bit unclear. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 5: Transition State Theory====&lt;br /&gt;
The Transition State Theory assumes that R&amp;lt;sub&amp;gt;cl&amp;lt;/sub&amp;gt; is that all trajectories with a KE greater than the activation energy will be reactive, however, our experimental has suggested that this is not true.&lt;br /&gt;
Transition state theory is based on classical mechanics, Quasi-equilibrium basically covers that if the atoms did not have enough energy to collide to form the TS, the reaction would not be feasible. However, in quantum mechanics, as long as the barrier has a finite amount of energy, the atoms can still tunnel across the barrier which means that the reaction could still be feasible even if the atoms do not collide enough energy to cross the energy barrier. &lt;br /&gt;
Quantum tunneling is minimal in TS theory, if quantum tunneling was present, the reaction rate would increase. &lt;br /&gt;
In transition state theory, it assumes that the step from TS to products is the rate-determining step, but  in reality, it might not be true, the reaction rate would. be decreased&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Make it clear which aspect of the table you are referring to. Quasi equilibrum refers to the concentration of TS remaming in relation to the concentration of reactant - i.e. the TS is treated as in chemical equilibria with the reactant. Barrier recrossing is not permitted in TST - is this observed in the above table? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===Exercise2: F-H-H system===&lt;br /&gt;
&lt;br /&gt;
====Part 1: PES inspection====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic, whereas HF + H is endothermic.&lt;br /&gt;
&lt;br /&gt;
H-H bond strength is weaker than the H-F bond. The energy absorbed to break the F-F bond is smaller than the energy needed to make the new bond H-F, the excess energy is then released as heat, so the reaction is exothermic. However, for HF + H, more energy is needed to break the H-F bond than to make the F-F bond, overall, energy is being absorbed rather than released, so the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok good answer just make it clear you are referring to the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 2: Transition State Approximation====&lt;br /&gt;
The approximate position of transition state:  r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=181.1 pm, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=74.488pm&lt;br /&gt;
The forces along AB and BC at this position are both 0. According to Hammond Postulate, an  exothermic reaction has an early TS, whereas an endothermic reaction has a late TS, therefore, one of the eigenvalues at TS is positive, another one is negative. In this case, the Hessian eigenvalues are -0.002 and +0.332.&lt;br /&gt;
As shown in the surface plot below, now it is at a saddle point which confirms the atoms are at the transition state.&lt;br /&gt;
[[File:Q7_xs2218_new.png|thumb|center|Surface Plot of transition state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok succinct answer. Hammond postulte could do with a reference. The Hessian value for BC indicates deviation from the actual TS. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 3: Activation Energy====&lt;br /&gt;
The transition state energy is reported as -433.981 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
A plot of energy vs time is plotted at TS as shown below.&lt;br /&gt;
[[File:Exe2_Q3_TSenergy.png|thumb|center|Energy vs Time plot at TS for F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
For the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the initial state energy is -435.059 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Activation energy can then be calculated as 1.08 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
[[File:Exe2_Q3_exoenergy.png|thumb|center|Energy vs Time plot at initial state for exothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
For the endothermic reaction HF + H, the initial state energy is -560.700 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Activation energy for this reaction is 126.02 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
[[File:Exe2_Q3_endoenergy.png|thumb|center|Energy vs Time plot at initial state for endothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
By locating a structure neighboring the TS, the plot of Energy vs time shows that the energy dropping clearly.&lt;br /&gt;
[[File:Exe2_Q3_endoenergy_new.png|thumb|center|Energy vs Time plot at the neighboring structure of  transition state for endothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
(The plot of the neighboring structure of TS for exothermic reaction is not shown because the difference is too small to be spotted.)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Great answer! Make sure to refer to the figures in the text. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 4: Release of reaction energy====&lt;br /&gt;
The release of reaction energy is basically a release of vibrational kinetic energy converted from potential energy. A contour plot of a reactive trajectory is shown below to illustrate.&lt;br /&gt;
[[File:Exe2_Q4_xs2218.png|thumb|center|A contour plot of a reactive trajectory in a F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
An experimental method to confirm it is IR spectrometry. IR absorption would have stronger overtones that measuring the transition from the first to second state, while IR emission measures the transition from the first to the ground state.&lt;br /&gt;
&lt;br /&gt;
====Part 5: Different modes of distribution of energy====&lt;br /&gt;
In general, vibrational energy is better than promoting endothermic reactions than exothermic reactions, whereas translational energy is better than promoting exothermic reactions than endothermic reactions.&lt;br /&gt;
When having translational energy, the atoms would bounce onto the potential wall and bounce back. When having vibrational energy, the atoms fall down the reaction channel and overcome the reaction barrier, forming the product.&lt;br /&gt;
&lt;br /&gt;
Plot 1 and 2 illustrate the situation when a huge amount of energy is put into the system on the H-H vibration, the trajectory moves from the left-hand side of the plot to the right-hand side.&lt;br /&gt;
[[File:Exe2_Q5_1.png|thumb|left|Plot 1: when the H-H vibration at low energy in an F-H-H system.]]&lt;br /&gt;
[[File:Exe2_Q5_2.png|thumb|center|Plot 2: when the H-H vibration at high energy in an F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When the momentum of F-H is increased slightly, the energy of the overall system is reduced by reducing the momentum of H-H which means the H-H vibrational energy is reduced, the trajectory plot below looks similar to plot 2 when there is high vibrational energy on H-H but with slightly lower F-H momentum. It further confirms that the exothermic reaction is promoted by translational energy better.&lt;br /&gt;
[[File:Exe2_Q5_3.png|thumb|center|Plot 3: when F-H momentum is  slightly increased and H-H momentum is reduced an F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
===References===&lt;br /&gt;
1. R. J. Silbey, R. A. Alberty, M. G. Bawendi Physical Chemistry, 4th ed, John Wiley &amp;amp; Sons, 2005.&lt;br /&gt;
&lt;br /&gt;
2. J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998, chapter 10&lt;br /&gt;
&lt;br /&gt;
3. K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987, chapter 4&lt;br /&gt;
&lt;br /&gt;
4. M. J. Pilling, P. W. Seakins Reaction Kinetics, 2nd ed., OUP, 1995, chapter 4&lt;br /&gt;
&lt;br /&gt;
5.Atkins, de Paula, Keeler, Physical Chemistry, 11th ed&lt;br /&gt;
&lt;br /&gt;
6. I. N. Levine, Physical Chemistry, McGraw-Hill, 4th ed&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:xs2218&amp;diff=812728</id>
		<title>MRD:xs2218</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:xs2218&amp;diff=812728"/>
		<updated>2020-06-04T12:32:29Z</updated>

		<summary type="html">&lt;p&gt;Rs6817: /* Part 2: Transition State Approximation */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Molecular Reaction Dynamic Lab==&lt;br /&gt;
===Exercise1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system===&lt;br /&gt;
&lt;br /&gt;
====Part 1: Definition of transition state====&lt;br /&gt;
On a potential energy surface diagram, the transition state is mathematically defined as a first-order saddle point, ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0. &lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.  To distinguish from the local minimum on the PES, the first-order saddle point is at a minimum in all directions except for one and the trajectories near the transition state roll towards reactants or products. See the surface plot below, the TS is at a saddle point.&lt;br /&gt;
[[File:Q1_xs2218.png|thumb|center|Surface plot of transition state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok, you could have included a description of the second derivative and what this tells us about the maxima and minima directions? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 2: Transition state approximation====&lt;br /&gt;
My best estimate of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;is 90.775pm, it is when the force along AB and BC is 0 KJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The atoms are not bonded at TS&lt;br /&gt;
The internuclear distance vs time plot shows 2 straight lines illustrating that when the atoms are at the transition state, the internuclear distance does not change, no such oscillating behavior where the 2 lines are wavy when not at TS.&lt;br /&gt;
[[File:Exe1 Q2.png|thumb|center|internuclear distance vs time plot at TS|350px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Okk, ensure that you refer to the figures numerically in the text and they are labelled as such i.e. Figure 1 shows X.  [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 3: Difference between MEP and Dynamics calculation type ====&lt;br /&gt;
As shown from the surface plots below, two different calculation types give different trajectories. The MEP shows the minimal energy path that any point on the path is at energy minimum in all directions perpendicular to the path which passes through at least one saddle point.  Looking at the plots from the same angle, the dynamic surface plot gives a wavy line coming out of the BC distance axis whereas the MEP surface plot gives a relatively straight line within the BC distance axis.&lt;br /&gt;
[[File:Exe1_Q3_mep_xs2218.png|thumb|left|Surface plot of MEP calculation type.|350px]]&lt;br /&gt;
[[File:Exe1_Q3_dynamics_xs2218.png|thumb|center|Surface plot of dynamics calculation type.|350px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Whilst this comparison is correct, you have not attributed what the wavy or straight lines correspond to. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 4: Reactive and unreactive trajectories====&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Table 1 r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74pm, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=200pm&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1 || -414.280 || yes || AB are bonded at first until B bonds with C and A moves away, prodct BC formed || [[File:table1_row1.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1 || -420.077 || No || AB is always bonded, no product formed || [[File:table1_row2.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1 || -5.1 || -413.977 || yes || AB are bonded at first until B is bonded with C and A moves away, prodct BC formed || [[File:table1_row3.png|150px]] || &lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.1 || -357.277 || No || AB are bonded at first until B bonds with C, but eventually B is back to bonded with A, C moves away, no product BC formed || [[File:table1_row4.png|150px]] ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1 || -10.6 || -349.477 || yes || AB are bonded at first until C approaches and B bonds with C, then B bonds with A again, eventually, B bonds with C and forms a product BC, A moves away|| [[File:table1_row5.png|150px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
In conclusion, trajectories starting with the same positions but with higher values of momenta would not always be reactive, although the total energy is getting more positive, therefore, the hypothesis is not supported&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|The descriptions for the table could do with a little more detail. In the last two trajectories we can see some clearly interesting behaviour with the barrier recrossing.Your conclusion is correct but could do with a little more detail as it is a bit unclear. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 5: Transition State Theory====&lt;br /&gt;
The Transition State Theory assumes that R&amp;lt;sub&amp;gt;cl&amp;lt;/sub&amp;gt; is that all trajectories with a KE greater than the activation energy will be reactive, however, our experimental has suggested that this is not true.&lt;br /&gt;
Transition state theory is based on classical mechanics, Quasi-equilibrium basically covers that if the atoms did not have enough energy to collide to form the TS, the reaction would not be feasible. However, in quantum mechanics, as long as the barrier has a finite amount of energy, the atoms can still tunnel across the barrier which means that the reaction could still be feasible even if the atoms do not collide enough energy to cross the energy barrier. &lt;br /&gt;
Quantum tunneling is minimal in TS theory, if quantum tunneling was present, the reaction rate would increase. &lt;br /&gt;
In transition state theory, it assumes that the step from TS to products is the rate-determining step, but  in reality, it might not be true, the reaction rate would. be decreased&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Make it clear which aspect of the table you are referring to. Quasi equilibrum refers to the concentration of TS remaming in relation to the concentration of reactant - i.e. the TS is treated as in chemical equilibria with the reactant. Barrier recrossing is not permitted in TST - is this observed in the above table? [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===Exercise2: F-H-H system===&lt;br /&gt;
&lt;br /&gt;
====Part 1: PES inspection====&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic, whereas HF + H is endothermic.&lt;br /&gt;
&lt;br /&gt;
H-H bond strength is weaker than the H-F bond. The energy absorbed to break the F-F bond is smaller than the energy needed to make the new bond H-F, the excess energy is then released as heat, so the reaction is exothermic. However, for HF + H, more energy is needed to break the H-F bond than to make the F-F bond, overall, energy is being absorbed rather than released, so the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok good answer just make it clear you are referring to the PES. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 2: Transition State Approximation====&lt;br /&gt;
The approximate position of transition state:  r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=181.1 pm, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=74.488pm&lt;br /&gt;
The forces along AB and BC at this position are both 0. According to Hammond Postulate, an  exothermic reaction has an early TS, whereas an endothermic reaction has a late TS, therefore, one of the eigenvalues at TS is positive, another one is negative. In this case, the Hessian eigenvalues are -0.002 and +0.332.&lt;br /&gt;
As shown in the surface plot below, now it is at a saddle point which confirms the atoms are at the transition state.&lt;br /&gt;
[[File:Q7_xs2218_new.png|thumb|center|Surface Plot of transition state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|green|Ok succinct answer. Hammond postulte could do with a reference. The Hessian value for BC indicates deviation from the actual TS. [[User:Rs6817|Rs6817]] ([[User talk:Rs6817|talk]]) 13:13, 4 June 2020 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Part 3: Activation Energy====&lt;br /&gt;
The transition state energy is reported as -433.981 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
A plot of energy vs time is plotted at TS as shown below.&lt;br /&gt;
[[File:Exe2_Q3_TSenergy.png|thumb|center|Energy vs Time plot at TS for F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
For the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the initial state energy is -435.059 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Activation energy can then be calculated as 1.08 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
[[File:Exe2_Q3_exoenergy.png|thumb|center|Energy vs Time plot at initial state for exothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
For the endothermic reaction HF + H, the initial state energy is -560.700 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Activation energy for this reaction is 126.02 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
[[File:Exe2_Q3_endoenergy.png|thumb|center|Energy vs Time plot at initial state for endothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
By locating a structure neighboring the TS, the plot of Energy vs time shows that the energy dropping clearly.&lt;br /&gt;
[[File:Exe2_Q3_endoenergy_new.png|thumb|center|Energy vs Time plot at the neighboring structure of  transition state for endothermic rxn.]]&lt;br /&gt;
&lt;br /&gt;
(The plot of the neighboring structure of TS for exothermic reaction is not shown because the difference is too small to be spotted.)&lt;br /&gt;
&lt;br /&gt;
====Part 4: Release of reaction energy====&lt;br /&gt;
The release of reaction energy is basically a release of vibrational kinetic energy converted from potential energy. A contour plot of a reactive trajectory is shown below to illustrate.&lt;br /&gt;
[[File:Exe2_Q4_xs2218.png|thumb|center|A contour plot of a reactive trajectory in a F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
An experimental method to confirm it is IR spectrometry. IR absorption would have stronger overtones that measuring the transition from the first to second state, while IR emission measures the transition from the first to the ground state.&lt;br /&gt;
&lt;br /&gt;
====Part 5: Different modes of distribution of energy====&lt;br /&gt;
In general, vibrational energy is better than promoting endothermic reactions than exothermic reactions, whereas translational energy is better than promoting exothermic reactions than endothermic reactions.&lt;br /&gt;
When having translational energy, the atoms would bounce onto the potential wall and bounce back. When having vibrational energy, the atoms fall down the reaction channel and overcome the reaction barrier, forming the product.&lt;br /&gt;
&lt;br /&gt;
Plot 1 and 2 illustrate the situation when a huge amount of energy is put into the system on the H-H vibration, the trajectory moves from the left-hand side of the plot to the right-hand side.&lt;br /&gt;
[[File:Exe2_Q5_1.png|thumb|left|Plot 1: when the H-H vibration at low energy in an F-H-H system.]]&lt;br /&gt;
[[File:Exe2_Q5_2.png|thumb|center|Plot 2: when the H-H vibration at high energy in an F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When the momentum of F-H is increased slightly, the energy of the overall system is reduced by reducing the momentum of H-H which means the H-H vibrational energy is reduced, the trajectory plot below looks similar to plot 2 when there is high vibrational energy on H-H but with slightly lower F-H momentum. It further confirms that the exothermic reaction is promoted by translational energy better.&lt;br /&gt;
[[File:Exe2_Q5_3.png|thumb|center|Plot 3: when F-H momentum is  slightly increased and H-H momentum is reduced an F-H-H system.]]&lt;br /&gt;
&lt;br /&gt;
===References===&lt;br /&gt;
1. R. J. Silbey, R. A. Alberty, M. G. Bawendi Physical Chemistry, 4th ed, John Wiley &amp;amp; Sons, 2005.&lt;br /&gt;
&lt;br /&gt;
2. J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics 2nd ed., Prentice-Hall, 1998, chapter 10&lt;br /&gt;
&lt;br /&gt;
3. K. J. Laidler Chemical Kinetics 3rd ed., Harper-Collins, 1987, chapter 4&lt;br /&gt;
&lt;br /&gt;
4. M. J. Pilling, P. W. Seakins Reaction Kinetics, 2nd ed., OUP, 1995, chapter 4&lt;br /&gt;
&lt;br /&gt;
5.Atkins, de Paula, Keeler, Physical Chemistry, 11th ed&lt;br /&gt;
&lt;br /&gt;
6. I. N. Levine, Physical Chemistry, McGraw-Hill, 4th ed&lt;/div&gt;</summary>
		<author><name>Rs6817</name></author>
	</entry>
</feed>