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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794112</id>
		<title>MRD:Jsr3217</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794112"/>
		<updated>2019-06-03T14:49:41Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Question 5: Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction for the reaction HF + H -&amp;gt; F + H2, and how this is influenced by the position of the transition state. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System  ==&lt;br /&gt;
&lt;br /&gt;
If we define H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; as A and BC in our system, as the hydrogen atom collides with the hydrogen molecule, provided H has enough momentum and thus enough energy, the system changes and is described as AB and C where AB is our new diatomic product (A,B and C are the same type of atom).  &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;
&lt;br /&gt;
The transition state for this triatomic collision is a saddle point located at the intersection of the two potential energy surfaces, one PES for the Hydrogen atom and 1 PES for the Hydrogen molecule. The transition state is also a maximum on the trajectory pathway.&lt;br /&gt;
&lt;br /&gt;
Firstly the transition state being a turning point has a derivative of 0 with respect to q. This is shown by the following equation: (∂V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) and (∂V(q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)=0. However being a saddle point, the transition state is also defined as the point in the surface plot where there is a minimum in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction but also a maximum in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction, where q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are orthogonal to each other . This is where we have to take into account the second derivative of the potential energy V with respect to q. Mathematically these results are expressed as ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;gt;0 and ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;lt;0. The former second order differential equation refers to the minimum point in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction and the latter second order differential equation refers to the maximum point in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction.&lt;br /&gt;
&lt;br /&gt;
The transition state can be distinguished from a local minimum of the potential energy surface as by definition a local minimum will only have one 2nd derivative of potential energy (with respect to q in this case) which is greater than 0. However the transition state, being a saddle point, is a point with 2 second derivatives of potential energy in two different directions, one which is greater than 0 and one which is less than 0. &lt;br /&gt;
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{{fontcolor|pink|I can tell from this explanation that you understand the shape of the TS on the PES however your discussion here is not quite complete as you haven&#039;t defined the directions q1 and q2 so you haven&#039;t fully defined the shape of the TS. A diagram with the vectors included would be really helpful here. In general diagrams are useful! Also, the below statement about the equal distances is true of this system only because it is a special case where the system is symmetrical. Be careful using this statement as it is not a generic description of a TS.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:23, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Original Surface Plot showing both Potential Energy Surfaces and the Trajectory Pathway:&lt;br /&gt;
&lt;br /&gt;
[[File:1st surface plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the point where the interatomic distances are equal i.e. when the bond length of A-B is equal to the bond length of B-C. This is when the A-B bond is forming to make the diatomic product AB and the B-C bond is breaking leaving C on its own. This is shown below in the contour plot:&lt;br /&gt;
[[File:1st contour plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== Question 2: What is 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;
&lt;br /&gt;
The position of the transition state can be found by varying the AB and BC distances, with both momentum values of AB and BC being 0, until no variation in the Internuclear Distances vs Time Plot is noticed or until a straight line in the plot is seen. No variation or oscillation in the plot means there are no vibrations which is what happens in the transition state. The distance at which no oscillation was seen was found to be at 0.90774 Å.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Internuclear Distance vs Time Plot at the transition state:&lt;br /&gt;
&lt;br /&gt;
[[File:2nd question graph 1.PNG]]&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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The plot with the MEP calculation shows a relatively short line with little variation in the y-axis (AB distance) however, the plot with the Dynamics calculation shows an oscillating line. The trajectory for the dynamics calculated plot is also longer in length than the MEP calculated plot. This is due to the MEP calculation not considering any vibrational modes therefore no oscillations are shown on the plot. In actuality, atoms have mass and momentum and so the vibrations of the hydrogen molecule are taken into account shown by the oscillations in the dynamics calculation plot. Thus the model with the dynamics calculation is the more accurate one.&lt;br /&gt;
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Plot with MEP Calculation:&lt;br /&gt;
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[[File:ACTUALMEP1.PNG]]&lt;br /&gt;
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Plot with Dynamics Calculation:&lt;br /&gt;
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[[File:ACTUALDYNAMIC.PNG]]&lt;br /&gt;
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{{fontcolor|pink|Your observations are valid, but can you think of why the MEP calculations shows no oscillations while the Dynamics calculation does, in terms of the calculation itself? An in depth understanding of the calculation process should aid in understanding the difference between the two methods. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:32, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 4: 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;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|+ Reactive or Unreactive Trajectories?&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the Trajectory !! Description &lt;br /&gt;
|-&lt;br /&gt;
| -1.25	|| -2.5	||-99.018 || Yes || [[File:1T.PNG]] ||Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products.|| &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.0	|| -100.456 || No || [[File:2T.PNG]] || Contour Plot shows that reaction does not occur as reactants don&#039;t have enough initial momentum and thus required (kinetic) energy to get over the activation energy barrier and reach the energy of the transition state. This is shown by the trajectory not reaching the transition state point and tailing back to the reactants. As the transition state isn&#039;t reached, the products aren&#039;t formed. || &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.5	|| -98.956|| Yes ||[[File:3T.PNG]] || Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products. The reaction is successful as the reactants have enough initial momentum and thus energy to reach the energy of the transition state. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.0	|| -84.956 || No || [[File:4T.PNG]] || Contour Plot shows although he reactants have enough initial momentum and thus energy to go through the transition state, the transition state collapses back into the reactants. This happens because of barrier recrossing. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.2	|| -83.416 || Yes || [[File:5T.PNG]] || Trajectory from contour plot shows that the reaction goes through/reaches the transition state point more than once. This occurs because of barrier recrossing again. However with these specific reaction conditions, the reaction does take place and the products are formed from the transition state. ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|What can you conclude overall from the table? Is the deciding factor in whether or not a reaction is successful as simple as a threshold activation energy, which if the molecules have they will definitely react?[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:34, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 5: State what are the main assumptions of Transition State Theory. 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;
&lt;br /&gt;
Transition State Theory assumes and tells us that states that &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; the transition state or activated complex in a reaction is in equilibrium with the reactants and once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. It also assumes the energy of the particles follows a Boltzmann distribution&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; but in this system since there are only 3 atoms in total for this triatomic collision there is no boltzmann distribution. As just mentioned, transition state theory assumes once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. However in contour plot 4 above where the trajectory shows that although the reaction goes through the transition state, the reactants are still reformed. This is because of barrier recrossing as mentioned above; with this present, the rate of this reaction, experimentally determined, would be lower than the reaction rate that the transition state theory would predict.&lt;br /&gt;
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{{fontcolor|pink|Great! You have demonstrated a really clear understanding here and explained your point clearly. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:36, 3 June 2019 (BST)}}&lt;br /&gt;
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== F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
=== Question 1: 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;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:D1.PNG]]&lt;br /&gt;
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The above surface plot shows the potential energy surface for the exothermic conversion of F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to HF and H. The potential energy well slopes downwards from the reactants to the products showing that the energy of the products is lower than the energy of reactants. This reaction is an exothermic one as the bond strength of HF, the product, is stronger than the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactant. This means that the energy released from the formation of the HF bond is greater than the energy required to break the H-H bond in the hydrogen reactant molecule making the overall reaction exothermic.&lt;br /&gt;
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[[File:D2endo.PNG]]&lt;br /&gt;
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The above surface plot shows the potential energy surface for the endothermic conversion of HF and H to H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F. This reaction is the reverse reaction of the exothermic conversion we&#039;ve just considered. This potenital energy well slopes upwards from the reactants to the products showing that the energy of the products is higher than the energy of reactants making the reaction endothermic. The energy released from the hydrogen molecule, the product, is less than the energy taken in to break in the H-F bond in the reactant making the overall reaction endothermic.&lt;br /&gt;
&lt;br /&gt;
=== Question 2: Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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Hammond&#039;s postulate essentially states that if 2 species are of similar energy they are of a similar structure. Thus in this reaction we can deduce that the transition state will be similar in structure to the reactants of the forward exothermic reaction, F and H2. By testing and varying the bond distances of F-H and H-H until the forces exterted on each other were 0 (characteristic in the transition state) the internuclear distances found were 1.811 Å for F-H and 0.745 for H-H Å.&lt;br /&gt;
&lt;br /&gt;
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{{fontcolor|pink|You should cite Hammond&#039;s postulate here.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:41, 3 June 2019 (BST)}}&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 easily calculated by taking away the reactant energy from the transition state energy. Using the internuclear distances of the atoms in the transition state calculated above in the settings function in the programme, the energy of the transition state was found to be -103.752 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;. The energy of the reactants, for the exothermic reaction for example, was found by inputting the normal bond length for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and making the distance between F and H relatively large so they&#039;re not interacting yielding the lowest energy for the reactants possible. From this the activation energies for the exothermic reaction was found to be 30.267 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; and the activation energy for the endothermic reaction was found to be 0.242 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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{{fontcolor|pink|This is quite a difficult and you could use plots to show the difference between energy of reactants and products which would better depict the activation energies and support your answers. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:43, 3 June 2019 (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 for the reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
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Due to the conservation of energy, all initial kinetic energy from the reactants&#039; momentum is converted and released as heat in the reaction once the products HF and H are formed. Due to the release of heat the surroundings temperature would increase as this is an exothermic reaction. This temperature change or increase in this case can be recorded by bomb calorimetry.&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 for the reaction HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For this endothermic reaction (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) there are two main modes of reactant energy to consider as the reactants approach the energy barrier/transition state point to form the products; these modes of energy are translational and vibrational energy. &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;Polanyi stated that for simple reactions described as an A + BC system, such as this H + HF system, if they have a late transition state, reactants with high vibrational energy is more effective for the reaction and its success, than reactants with high translational energy. This is because for a late transition state reaction, reactant molecules with high vibrational energy, if in the correct orientation, can vibrate their way to the top of the barrier, passing through the transition state forming the products successfully; however, if the reactants had high translational energy, in trying to reach the top of the energy barrier, they would just collide into the inner wall of the potential energy well and return to where they came from. This reaction being considered here (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) is an endothermic reaction with a late transition state as shown by the surface plot discussed earlier. Therefore to maximise the efficiency and the success of this reaction, reactants should have high vibrational energy. Polanyi also implied, that in this type of reaction (endothermic and late transition state), the products are likely to have high translational energy if the reaction effectively occurs with high vibrational energy reactants.&lt;br /&gt;
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The reaction showing highest efficiency and most effectiveness for its success was then modelled; high vibrational energy was inputted in the settings function for the molecule HF and high initial momentum of the incoming hydrogen atom for the collision was also inputted. However, unfortunately no such combination of momenta and bond length values were found that yielded a successful reaction, but below shows a contour plot with high vibrational energy in the reactants as shown by the oscillating trajectory which is what is needed to ensure high efficiency of this late transition state endothermic reaction.&lt;br /&gt;
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[[File:Loooool.png]]&lt;br /&gt;
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{{fontcolor|pink|Maybe you have a high vibrational energy but also a high translational energy? There seem to be large amounts of space covered in between each step (big gaps between the black dots) so perhaps the translational energy was too high. Also, a full investigation of Polanyi&#039;s rules would show a reactive trajectory of high vib energy (which does exist but you have not found), an unreactive trajectory of high trans energy, and also for an exothermic reaction these two conditions with opposite observations. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:49, 3 June 2019 (BST)}}&lt;br /&gt;
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== References  ==&lt;br /&gt;
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&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; P. Atkins, J. De Paula, (n.d.). Physical chemistry. 7th edition.&lt;br /&gt;
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&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics Prentice-Hall.&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794111</id>
		<title>MRD:Jsr3217</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794111"/>
		<updated>2019-06-03T14:43:11Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Question 3: Report the activation energy for both reactions. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System  ==&lt;br /&gt;
&lt;br /&gt;
If we define H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; as A and BC in our system, as the hydrogen atom collides with the hydrogen molecule, provided H has enough momentum and thus enough energy, the system changes and is described as AB and C where AB is our new diatomic product (A,B and C are the same type of atom).  &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;
&lt;br /&gt;
The transition state for this triatomic collision is a saddle point located at the intersection of the two potential energy surfaces, one PES for the Hydrogen atom and 1 PES for the Hydrogen molecule. The transition state is also a maximum on the trajectory pathway.&lt;br /&gt;
&lt;br /&gt;
Firstly the transition state being a turning point has a derivative of 0 with respect to q. This is shown by the following equation: (∂V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) and (∂V(q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)=0. However being a saddle point, the transition state is also defined as the point in the surface plot where there is a minimum in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction but also a maximum in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction, where q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are orthogonal to each other . This is where we have to take into account the second derivative of the potential energy V with respect to q. Mathematically these results are expressed as ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;gt;0 and ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;lt;0. The former second order differential equation refers to the minimum point in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction and the latter second order differential equation refers to the maximum point in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction.&lt;br /&gt;
&lt;br /&gt;
The transition state can be distinguished from a local minimum of the potential energy surface as by definition a local minimum will only have one 2nd derivative of potential energy (with respect to q in this case) which is greater than 0. However the transition state, being a saddle point, is a point with 2 second derivatives of potential energy in two different directions, one which is greater than 0 and one which is less than 0. &lt;br /&gt;
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{{fontcolor|pink|I can tell from this explanation that you understand the shape of the TS on the PES however your discussion here is not quite complete as you haven&#039;t defined the directions q1 and q2 so you haven&#039;t fully defined the shape of the TS. A diagram with the vectors included would be really helpful here. In general diagrams are useful! Also, the below statement about the equal distances is true of this system only because it is a special case where the system is symmetrical. Be careful using this statement as it is not a generic description of a TS.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:23, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Original Surface Plot showing both Potential Energy Surfaces and the Trajectory Pathway:&lt;br /&gt;
&lt;br /&gt;
[[File:1st surface plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the point where the interatomic distances are equal i.e. when the bond length of A-B is equal to the bond length of B-C. This is when the A-B bond is forming to make the diatomic product AB and the B-C bond is breaking leaving C on its own. This is shown below in the contour plot:&lt;br /&gt;
[[File:1st contour plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== Question 2: What is 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;
&lt;br /&gt;
The position of the transition state can be found by varying the AB and BC distances, with both momentum values of AB and BC being 0, until no variation in the Internuclear Distances vs Time Plot is noticed or until a straight line in the plot is seen. No variation or oscillation in the plot means there are no vibrations which is what happens in the transition state. The distance at which no oscillation was seen was found to be at 0.90774 Å.&lt;br /&gt;
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Internuclear Distance vs Time Plot at the transition state:&lt;br /&gt;
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[[File:2nd question graph 1.PNG]]&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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The plot with the MEP calculation shows a relatively short line with little variation in the y-axis (AB distance) however, the plot with the Dynamics calculation shows an oscillating line. The trajectory for the dynamics calculated plot is also longer in length than the MEP calculated plot. This is due to the MEP calculation not considering any vibrational modes therefore no oscillations are shown on the plot. In actuality, atoms have mass and momentum and so the vibrations of the hydrogen molecule are taken into account shown by the oscillations in the dynamics calculation plot. Thus the model with the dynamics calculation is the more accurate one.&lt;br /&gt;
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Plot with MEP Calculation:&lt;br /&gt;
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[[File:ACTUALMEP1.PNG]]&lt;br /&gt;
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Plot with Dynamics Calculation:&lt;br /&gt;
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[[File:ACTUALDYNAMIC.PNG]]&lt;br /&gt;
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{{fontcolor|pink|Your observations are valid, but can you think of why the MEP calculations shows no oscillations while the Dynamics calculation does, in terms of the calculation itself? An in depth understanding of the calculation process should aid in understanding the difference between the two methods. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:32, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 4: 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;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|+ Reactive or Unreactive Trajectories?&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the Trajectory !! Description &lt;br /&gt;
|-&lt;br /&gt;
| -1.25	|| -2.5	||-99.018 || Yes || [[File:1T.PNG]] ||Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products.|| &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.0	|| -100.456 || No || [[File:2T.PNG]] || Contour Plot shows that reaction does not occur as reactants don&#039;t have enough initial momentum and thus required (kinetic) energy to get over the activation energy barrier and reach the energy of the transition state. This is shown by the trajectory not reaching the transition state point and tailing back to the reactants. As the transition state isn&#039;t reached, the products aren&#039;t formed. || &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.5	|| -98.956|| Yes ||[[File:3T.PNG]] || Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products. The reaction is successful as the reactants have enough initial momentum and thus energy to reach the energy of the transition state. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.0	|| -84.956 || No || [[File:4T.PNG]] || Contour Plot shows although he reactants have enough initial momentum and thus energy to go through the transition state, the transition state collapses back into the reactants. This happens because of barrier recrossing. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.2	|| -83.416 || Yes || [[File:5T.PNG]] || Trajectory from contour plot shows that the reaction goes through/reaches the transition state point more than once. This occurs because of barrier recrossing again. However with these specific reaction conditions, the reaction does take place and the products are formed from the transition state. ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|What can you conclude overall from the table? Is the deciding factor in whether or not a reaction is successful as simple as a threshold activation energy, which if the molecules have they will definitely react?[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:34, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 5: State what are the main assumptions of Transition State Theory. 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;
&lt;br /&gt;
Transition State Theory assumes and tells us that states that &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; the transition state or activated complex in a reaction is in equilibrium with the reactants and once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. It also assumes the energy of the particles follows a Boltzmann distribution&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; but in this system since there are only 3 atoms in total for this triatomic collision there is no boltzmann distribution. As just mentioned, transition state theory assumes once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. However in contour plot 4 above where the trajectory shows that although the reaction goes through the transition state, the reactants are still reformed. This is because of barrier recrossing as mentioned above; with this present, the rate of this reaction, experimentally determined, would be lower than the reaction rate that the transition state theory would predict.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Great! You have demonstrated a really clear understanding here and explained your point clearly. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:36, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
=== Question 1: 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;br /&gt;
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[[File:D1.PNG]]&lt;br /&gt;
&lt;br /&gt;
The above surface plot shows the potential energy surface for the exothermic conversion of F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to HF and H. The potential energy well slopes downwards from the reactants to the products showing that the energy of the products is lower than the energy of reactants. This reaction is an exothermic one as the bond strength of HF, the product, is stronger than the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactant. This means that the energy released from the formation of the HF bond is greater than the energy required to break the H-H bond in the hydrogen reactant molecule making the overall reaction exothermic.&lt;br /&gt;
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[[File:D2endo.PNG]]&lt;br /&gt;
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The above surface plot shows the potential energy surface for the endothermic conversion of HF and H to H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F. This reaction is the reverse reaction of the exothermic conversion we&#039;ve just considered. This potenital energy well slopes upwards from the reactants to the products showing that the energy of the products is higher than the energy of reactants making the reaction endothermic. The energy released from the hydrogen molecule, the product, is less than the energy taken in to break in the H-F bond in the reactant making the overall reaction endothermic.&lt;br /&gt;
&lt;br /&gt;
=== Question 2: Locate the approximate position of the transition state. ===&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate essentially states that if 2 species are of similar energy they are of a similar structure. Thus in this reaction we can deduce that the transition state will be similar in structure to the reactants of the forward exothermic reaction, F and H2. By testing and varying the bond distances of F-H and H-H until the forces exterted on each other were 0 (characteristic in the transition state) the internuclear distances found were 1.811 Å for F-H and 0.745 for H-H Å.&lt;br /&gt;
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{{fontcolor|pink|You should cite Hammond&#039;s postulate here.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:41, 3 June 2019 (BST)}}&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 easily calculated by taking away the reactant energy from the transition state energy. Using the internuclear distances of the atoms in the transition state calculated above in the settings function in the programme, the energy of the transition state was found to be -103.752 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;. The energy of the reactants, for the exothermic reaction for example, was found by inputting the normal bond length for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and making the distance between F and H relatively large so they&#039;re not interacting yielding the lowest energy for the reactants possible. From this the activation energies for the exothermic reaction was found to be 30.267 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; and the activation energy for the endothermic reaction was found to be 0.242 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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{{fontcolor|pink|This is quite a difficult and you could use plots to show the difference between energy of reactants and products which would better depict the activation energies and support your answers. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:43, 3 June 2019 (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 for the reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
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Due to the conservation of energy, all initial kinetic energy from the reactants&#039; momentum is converted and released as heat in the reaction once the products HF and H are formed. Due to the release of heat the surroundings temperature would increase as this is an exothermic reaction. This temperature change or increase in this case can be recorded by bomb calorimetry.&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 for the reaction HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
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For this endothermic reaction (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) there are two main modes of reactant energy to consider as the reactants approach the energy barrier/transition state point to form the products; these modes of energy are translational and vibrational energy. &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;Polanyi stated that for simple reactions described as an A + BC system, such as this H + HF system, if they have a late transition state, reactants with high vibrational energy is more effective for the reaction and its success, than reactants with high translational energy. This is because for a late transition state reaction, reactant molecules with high vibrational energy, if in the correct orientation, can vibrate their way to the top of the barrier, passing through the transition state forming the products successfully; however, if the reactants had high translational energy, in trying to reach the top of the energy barrier, they would just collide into the inner wall of the potential energy well and return to where they came from. This reaction being considered here (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) is an endothermic reaction with a late transition state as shown by the surface plot discussed earlier. Therefore to maximise the efficiency and the success of this reaction, reactants should have high vibrational energy. Polanyi also implied, that in this type of reaction (endothermic and late transition state), the products are likely to have high translational energy if the reaction effectively occurs with high vibrational energy reactants.&lt;br /&gt;
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The reaction showing highest efficiency and most effectiveness for its success was then modelled; high vibrational energy was inputted in the settings function for the molecule HF and high initial momentum of the incoming hydrogen atom for the collision was also inputted. However, unfortunately no such combination of momenta and bond length values were found that yielded a successful reaction, but below shows a contour plot with high vibrational energy in the reactants as shown by the oscillating trajectory which is what is needed to ensure high efficiency of this late transition state endothermic reaction.&lt;br /&gt;
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[[File:Loooool.png]]&lt;br /&gt;
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== References  ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; P. Atkins, J. De Paula, (n.d.). Physical chemistry. 7th edition.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics Prentice-Hall.&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794110</id>
		<title>MRD:Jsr3217</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794110"/>
		<updated>2019-06-03T14:41:59Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Question 2: Locate the approximate position of the transition state. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System  ==&lt;br /&gt;
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If we define H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; as A and BC in our system, as the hydrogen atom collides with the hydrogen molecule, provided H has enough momentum and thus enough energy, the system changes and is described as AB and C where AB is our new diatomic product (A,B and C are the same type of atom).  &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;
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The transition state for this triatomic collision is a saddle point located at the intersection of the two potential energy surfaces, one PES for the Hydrogen atom and 1 PES for the Hydrogen molecule. The transition state is also a maximum on the trajectory pathway.&lt;br /&gt;
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Firstly the transition state being a turning point has a derivative of 0 with respect to q. This is shown by the following equation: (∂V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) and (∂V(q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)=0. However being a saddle point, the transition state is also defined as the point in the surface plot where there is a minimum in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction but also a maximum in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction, where q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are orthogonal to each other . This is where we have to take into account the second derivative of the potential energy V with respect to q. Mathematically these results are expressed as ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;gt;0 and ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;lt;0. The former second order differential equation refers to the minimum point in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction and the latter second order differential equation refers to the maximum point in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction.&lt;br /&gt;
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The transition state can be distinguished from a local minimum of the potential energy surface as by definition a local minimum will only have one 2nd derivative of potential energy (with respect to q in this case) which is greater than 0. However the transition state, being a saddle point, is a point with 2 second derivatives of potential energy in two different directions, one which is greater than 0 and one which is less than 0. &lt;br /&gt;
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{{fontcolor|pink|I can tell from this explanation that you understand the shape of the TS on the PES however your discussion here is not quite complete as you haven&#039;t defined the directions q1 and q2 so you haven&#039;t fully defined the shape of the TS. A diagram with the vectors included would be really helpful here. In general diagrams are useful! Also, the below statement about the equal distances is true of this system only because it is a special case where the system is symmetrical. Be careful using this statement as it is not a generic description of a TS.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:23, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Original Surface Plot showing both Potential Energy Surfaces and the Trajectory Pathway:&lt;br /&gt;
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[[File:1st surface plot.PNG]]&lt;br /&gt;
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The transition state is located at the point where the interatomic distances are equal i.e. when the bond length of A-B is equal to the bond length of B-C. This is when the A-B bond is forming to make the diatomic product AB and the B-C bond is breaking leaving C on its own. This is shown below in the contour plot:&lt;br /&gt;
[[File:1st contour plot.PNG]]&lt;br /&gt;
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=== Question 2: What is 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;
&lt;br /&gt;
The position of the transition state can be found by varying the AB and BC distances, with both momentum values of AB and BC being 0, until no variation in the Internuclear Distances vs Time Plot is noticed or until a straight line in the plot is seen. No variation or oscillation in the plot means there are no vibrations which is what happens in the transition state. The distance at which no oscillation was seen was found to be at 0.90774 Å.&lt;br /&gt;
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Internuclear Distance vs Time Plot at the transition state:&lt;br /&gt;
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[[File:2nd question graph 1.PNG]]&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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The plot with the MEP calculation shows a relatively short line with little variation in the y-axis (AB distance) however, the plot with the Dynamics calculation shows an oscillating line. The trajectory for the dynamics calculated plot is also longer in length than the MEP calculated plot. This is due to the MEP calculation not considering any vibrational modes therefore no oscillations are shown on the plot. In actuality, atoms have mass and momentum and so the vibrations of the hydrogen molecule are taken into account shown by the oscillations in the dynamics calculation plot. Thus the model with the dynamics calculation is the more accurate one.&lt;br /&gt;
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Plot with MEP Calculation:&lt;br /&gt;
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[[File:ACTUALMEP1.PNG]]&lt;br /&gt;
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Plot with Dynamics Calculation:&lt;br /&gt;
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[[File:ACTUALDYNAMIC.PNG]]&lt;br /&gt;
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{{fontcolor|pink|Your observations are valid, but can you think of why the MEP calculations shows no oscillations while the Dynamics calculation does, in terms of the calculation itself? An in depth understanding of the calculation process should aid in understanding the difference between the two methods. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:32, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 4: 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;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|+ Reactive or Unreactive Trajectories?&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the Trajectory !! Description &lt;br /&gt;
|-&lt;br /&gt;
| -1.25	|| -2.5	||-99.018 || Yes || [[File:1T.PNG]] ||Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products.|| &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.0	|| -100.456 || No || [[File:2T.PNG]] || Contour Plot shows that reaction does not occur as reactants don&#039;t have enough initial momentum and thus required (kinetic) energy to get over the activation energy barrier and reach the energy of the transition state. This is shown by the trajectory not reaching the transition state point and tailing back to the reactants. As the transition state isn&#039;t reached, the products aren&#039;t formed. || &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.5	|| -98.956|| Yes ||[[File:3T.PNG]] || Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products. The reaction is successful as the reactants have enough initial momentum and thus energy to reach the energy of the transition state. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.0	|| -84.956 || No || [[File:4T.PNG]] || Contour Plot shows although he reactants have enough initial momentum and thus energy to go through the transition state, the transition state collapses back into the reactants. This happens because of barrier recrossing. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.2	|| -83.416 || Yes || [[File:5T.PNG]] || Trajectory from contour plot shows that the reaction goes through/reaches the transition state point more than once. This occurs because of barrier recrossing again. However with these specific reaction conditions, the reaction does take place and the products are formed from the transition state. ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|What can you conclude overall from the table? Is the deciding factor in whether or not a reaction is successful as simple as a threshold activation energy, which if the molecules have they will definitely react?[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:34, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 5: State what are the main assumptions of Transition State Theory. 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;
&lt;br /&gt;
Transition State Theory assumes and tells us that states that &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; the transition state or activated complex in a reaction is in equilibrium with the reactants and once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. It also assumes the energy of the particles follows a Boltzmann distribution&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; but in this system since there are only 3 atoms in total for this triatomic collision there is no boltzmann distribution. As just mentioned, transition state theory assumes once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. However in contour plot 4 above where the trajectory shows that although the reaction goes through the transition state, the reactants are still reformed. This is because of barrier recrossing as mentioned above; with this present, the rate of this reaction, experimentally determined, would be lower than the reaction rate that the transition state theory would predict.&lt;br /&gt;
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{{fontcolor|pink|Great! You have demonstrated a really clear understanding here and explained your point clearly. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:36, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
=== Question 1: 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;br /&gt;
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[[File:D1.PNG]]&lt;br /&gt;
&lt;br /&gt;
The above surface plot shows the potential energy surface for the exothermic conversion of F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to HF and H. The potential energy well slopes downwards from the reactants to the products showing that the energy of the products is lower than the energy of reactants. This reaction is an exothermic one as the bond strength of HF, the product, is stronger than the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactant. This means that the energy released from the formation of the HF bond is greater than the energy required to break the H-H bond in the hydrogen reactant molecule making the overall reaction exothermic.&lt;br /&gt;
&lt;br /&gt;
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[[File:D2endo.PNG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The above surface plot shows the potential energy surface for the endothermic conversion of HF and H to H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F. This reaction is the reverse reaction of the exothermic conversion we&#039;ve just considered. This potenital energy well slopes upwards from the reactants to the products showing that the energy of the products is higher than the energy of reactants making the reaction endothermic. The energy released from the hydrogen molecule, the product, is less than the energy taken in to break in the H-F bond in the reactant making the overall reaction endothermic.&lt;br /&gt;
&lt;br /&gt;
=== Question 2: Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate essentially states that if 2 species are of similar energy they are of a similar structure. Thus in this reaction we can deduce that the transition state will be similar in structure to the reactants of the forward exothermic reaction, F and H2. By testing and varying the bond distances of F-H and H-H until the forces exterted on each other were 0 (characteristic in the transition state) the internuclear distances found were 1.811 Å for F-H and 0.745 for H-H Å.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|You should cite Hammond&#039;s postulate here.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:41, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 3: Report the activation energy for both reactions. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The activation energy can be easily calculated by taking away the reactant energy from the transition state energy. Using the internuclear distances of the atoms in the transition state calculated above in the settings function in the programme, the energy of the transition state was found to be -103.752 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;. The energy of the reactants, for the exothermic reaction for example, was found by inputting the normal bond length for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and making the distance between F and H relatively large so they&#039;re not interacting yielding the lowest energy for the reactants possible. From this the activation energies for the exothermic reaction was found to be 30.267 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; and the activation energy for the endothermic reaction was found to be 0.242 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;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 for the reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
&lt;br /&gt;
Due to the conservation of energy, all initial kinetic energy from the reactants&#039; momentum is converted and released as heat in the reaction once the products HF and H are formed. Due to the release of heat the surroundings temperature would increase as this is an exothermic reaction. This temperature change or increase in this case can be recorded by bomb calorimetry.&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 for the reaction HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For this endothermic reaction (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) there are two main modes of reactant energy to consider as the reactants approach the energy barrier/transition state point to form the products; these modes of energy are translational and vibrational energy. &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;Polanyi stated that for simple reactions described as an A + BC system, such as this H + HF system, if they have a late transition state, reactants with high vibrational energy is more effective for the reaction and its success, than reactants with high translational energy. This is because for a late transition state reaction, reactant molecules with high vibrational energy, if in the correct orientation, can vibrate their way to the top of the barrier, passing through the transition state forming the products successfully; however, if the reactants had high translational energy, in trying to reach the top of the energy barrier, they would just collide into the inner wall of the potential energy well and return to where they came from. This reaction being considered here (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) is an endothermic reaction with a late transition state as shown by the surface plot discussed earlier. Therefore to maximise the efficiency and the success of this reaction, reactants should have high vibrational energy. Polanyi also implied, that in this type of reaction (endothermic and late transition state), the products are likely to have high translational energy if the reaction effectively occurs with high vibrational energy reactants.&lt;br /&gt;
&lt;br /&gt;
The reaction showing highest efficiency and most effectiveness for its success was then modelled; high vibrational energy was inputted in the settings function for the molecule HF and high initial momentum of the incoming hydrogen atom for the collision was also inputted. However, unfortunately no such combination of momenta and bond length values were found that yielded a successful reaction, but below shows a contour plot with high vibrational energy in the reactants as shown by the oscillating trajectory which is what is needed to ensure high efficiency of this late transition state endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Loooool.png]]&lt;br /&gt;
&lt;br /&gt;
== References  ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; P. Atkins, J. De Paula, (n.d.). Physical chemistry. 7th edition.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics Prentice-Hall.&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794109</id>
		<title>MRD:Jsr3217</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794109"/>
		<updated>2019-06-03T14:36:04Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Question 5: State what are the main assumptions of Transition State Theory. 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;== H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System  ==&lt;br /&gt;
&lt;br /&gt;
If we define H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; as A and BC in our system, as the hydrogen atom collides with the hydrogen molecule, provided H has enough momentum and thus enough energy, the system changes and is described as AB and C where AB is our new diatomic product (A,B and C are the same type of atom).  &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;
&lt;br /&gt;
The transition state for this triatomic collision is a saddle point located at the intersection of the two potential energy surfaces, one PES for the Hydrogen atom and 1 PES for the Hydrogen molecule. The transition state is also a maximum on the trajectory pathway.&lt;br /&gt;
&lt;br /&gt;
Firstly the transition state being a turning point has a derivative of 0 with respect to q. This is shown by the following equation: (∂V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) and (∂V(q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)=0. However being a saddle point, the transition state is also defined as the point in the surface plot where there is a minimum in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction but also a maximum in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction, where q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are orthogonal to each other . This is where we have to take into account the second derivative of the potential energy V with respect to q. Mathematically these results are expressed as ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;gt;0 and ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;lt;0. The former second order differential equation refers to the minimum point in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction and the latter second order differential equation refers to the maximum point in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction.&lt;br /&gt;
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The transition state can be distinguished from a local minimum of the potential energy surface as by definition a local minimum will only have one 2nd derivative of potential energy (with respect to q in this case) which is greater than 0. However the transition state, being a saddle point, is a point with 2 second derivatives of potential energy in two different directions, one which is greater than 0 and one which is less than 0. &lt;br /&gt;
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{{fontcolor|pink|I can tell from this explanation that you understand the shape of the TS on the PES however your discussion here is not quite complete as you haven&#039;t defined the directions q1 and q2 so you haven&#039;t fully defined the shape of the TS. A diagram with the vectors included would be really helpful here. In general diagrams are useful! Also, the below statement about the equal distances is true of this system only because it is a special case where the system is symmetrical. Be careful using this statement as it is not a generic description of a TS.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:23, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Original Surface Plot showing both Potential Energy Surfaces and the Trajectory Pathway:&lt;br /&gt;
&lt;br /&gt;
[[File:1st surface plot.PNG]]&lt;br /&gt;
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The transition state is located at the point where the interatomic distances are equal i.e. when the bond length of A-B is equal to the bond length of B-C. This is when the A-B bond is forming to make the diatomic product AB and the B-C bond is breaking leaving C on its own. This is shown below in the contour plot:&lt;br /&gt;
[[File:1st contour plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== Question 2: What is 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;
&lt;br /&gt;
The position of the transition state can be found by varying the AB and BC distances, with both momentum values of AB and BC being 0, until no variation in the Internuclear Distances vs Time Plot is noticed or until a straight line in the plot is seen. No variation or oscillation in the plot means there are no vibrations which is what happens in the transition state. The distance at which no oscillation was seen was found to be at 0.90774 Å.&lt;br /&gt;
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Internuclear Distance vs Time Plot at the transition state:&lt;br /&gt;
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[[File:2nd question graph 1.PNG]]&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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The plot with the MEP calculation shows a relatively short line with little variation in the y-axis (AB distance) however, the plot with the Dynamics calculation shows an oscillating line. The trajectory for the dynamics calculated plot is also longer in length than the MEP calculated plot. This is due to the MEP calculation not considering any vibrational modes therefore no oscillations are shown on the plot. In actuality, atoms have mass and momentum and so the vibrations of the hydrogen molecule are taken into account shown by the oscillations in the dynamics calculation plot. Thus the model with the dynamics calculation is the more accurate one.&lt;br /&gt;
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Plot with MEP Calculation:&lt;br /&gt;
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[[File:ACTUALMEP1.PNG]]&lt;br /&gt;
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Plot with Dynamics Calculation:&lt;br /&gt;
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[[File:ACTUALDYNAMIC.PNG]]&lt;br /&gt;
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{{fontcolor|pink|Your observations are valid, but can you think of why the MEP calculations shows no oscillations while the Dynamics calculation does, in terms of the calculation itself? An in depth understanding of the calculation process should aid in understanding the difference between the two methods. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:32, 3 June 2019 (BST)}}&lt;br /&gt;
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=== Question 4: 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;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|+ Reactive or Unreactive Trajectories?&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the Trajectory !! Description &lt;br /&gt;
|-&lt;br /&gt;
| -1.25	|| -2.5	||-99.018 || Yes || [[File:1T.PNG]] ||Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products.|| &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.0	|| -100.456 || No || [[File:2T.PNG]] || Contour Plot shows that reaction does not occur as reactants don&#039;t have enough initial momentum and thus required (kinetic) energy to get over the activation energy barrier and reach the energy of the transition state. This is shown by the trajectory not reaching the transition state point and tailing back to the reactants. As the transition state isn&#039;t reached, the products aren&#039;t formed. || &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.5	|| -98.956|| Yes ||[[File:3T.PNG]] || Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products. The reaction is successful as the reactants have enough initial momentum and thus energy to reach the energy of the transition state. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.0	|| -84.956 || No || [[File:4T.PNG]] || Contour Plot shows although he reactants have enough initial momentum and thus energy to go through the transition state, the transition state collapses back into the reactants. This happens because of barrier recrossing. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.2	|| -83.416 || Yes || [[File:5T.PNG]] || Trajectory from contour plot shows that the reaction goes through/reaches the transition state point more than once. This occurs because of barrier recrossing again. However with these specific reaction conditions, the reaction does take place and the products are formed from the transition state. ||&lt;br /&gt;
|}&lt;br /&gt;
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{{fontcolor|pink|What can you conclude overall from the table? Is the deciding factor in whether or not a reaction is successful as simple as a threshold activation energy, which if the molecules have they will definitely react?[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:34, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 5: State what are the main assumptions of Transition State Theory. 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;
&lt;br /&gt;
Transition State Theory assumes and tells us that states that &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; the transition state or activated complex in a reaction is in equilibrium with the reactants and once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. It also assumes the energy of the particles follows a Boltzmann distribution&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; but in this system since there are only 3 atoms in total for this triatomic collision there is no boltzmann distribution. As just mentioned, transition state theory assumes once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. However in contour plot 4 above where the trajectory shows that although the reaction goes through the transition state, the reactants are still reformed. This is because of barrier recrossing as mentioned above; with this present, the rate of this reaction, experimentally determined, would be lower than the reaction rate that the transition state theory would predict.&lt;br /&gt;
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{{fontcolor|pink|Great! You have demonstrated a really clear understanding here and explained your point clearly. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:36, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
=== Question 1: 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;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:D1.PNG]]&lt;br /&gt;
&lt;br /&gt;
The above surface plot shows the potential energy surface for the exothermic conversion of F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to HF and H. The potential energy well slopes downwards from the reactants to the products showing that the energy of the products is lower than the energy of reactants. This reaction is an exothermic one as the bond strength of HF, the product, is stronger than the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactant. This means that the energy released from the formation of the HF bond is greater than the energy required to break the H-H bond in the hydrogen reactant molecule making the overall reaction exothermic.&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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[[File:D2endo.PNG]]&lt;br /&gt;
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The above surface plot shows the potential energy surface for the endothermic conversion of HF and H to H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F. This reaction is the reverse reaction of the exothermic conversion we&#039;ve just considered. This potenital energy well slopes upwards from the reactants to the products showing that the energy of the products is higher than the energy of reactants making the reaction endothermic. The energy released from the hydrogen molecule, the product, is less than the energy taken in to break in the H-F bond in the reactant making the overall reaction endothermic.&lt;br /&gt;
&lt;br /&gt;
=== Question 2: Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate essentially states that if 2 species are of similar energy they are of a similar structure. Thus in this reaction we can deduce that the transition state will be similar in structure to the reactants of the forward exothermic reaction, F and H2. By testing and varying the bond distances of F-H and H-H until the forces exterted on each other were 0 (characteristic in the transition state) the internuclear distances found were 1.811 Å for F-H and 0.745 for H-H Å.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Question 3: Report the activation energy for both reactions. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The activation energy can be easily calculated by taking away the reactant energy from the transition state energy. Using the internuclear distances of the atoms in the transition state calculated above in the settings function in the programme, the energy of the transition state was found to be -103.752 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;. The energy of the reactants, for the exothermic reaction for example, was found by inputting the normal bond length for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and making the distance between F and H relatively large so they&#039;re not interacting yielding the lowest energy for the reactants possible. From this the activation energies for the exothermic reaction was found to be 30.267 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; and the activation energy for the endothermic reaction was found to be 0.242 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;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 for the reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
&lt;br /&gt;
Due to the conservation of energy, all initial kinetic energy from the reactants&#039; momentum is converted and released as heat in the reaction once the products HF and H are formed. Due to the release of heat the surroundings temperature would increase as this is an exothermic reaction. This temperature change or increase in this case can be recorded by bomb calorimetry.&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 for the reaction HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For this endothermic reaction (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) there are two main modes of reactant energy to consider as the reactants approach the energy barrier/transition state point to form the products; these modes of energy are translational and vibrational energy. &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;Polanyi stated that for simple reactions described as an A + BC system, such as this H + HF system, if they have a late transition state, reactants with high vibrational energy is more effective for the reaction and its success, than reactants with high translational energy. This is because for a late transition state reaction, reactant molecules with high vibrational energy, if in the correct orientation, can vibrate their way to the top of the barrier, passing through the transition state forming the products successfully; however, if the reactants had high translational energy, in trying to reach the top of the energy barrier, they would just collide into the inner wall of the potential energy well and return to where they came from. This reaction being considered here (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) is an endothermic reaction with a late transition state as shown by the surface plot discussed earlier. Therefore to maximise the efficiency and the success of this reaction, reactants should have high vibrational energy. Polanyi also implied, that in this type of reaction (endothermic and late transition state), the products are likely to have high translational energy if the reaction effectively occurs with high vibrational energy reactants.&lt;br /&gt;
&lt;br /&gt;
The reaction showing highest efficiency and most effectiveness for its success was then modelled; high vibrational energy was inputted in the settings function for the molecule HF and high initial momentum of the incoming hydrogen atom for the collision was also inputted. However, unfortunately no such combination of momenta and bond length values were found that yielded a successful reaction, but below shows a contour plot with high vibrational energy in the reactants as shown by the oscillating trajectory which is what is needed to ensure high efficiency of this late transition state endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Loooool.png]]&lt;br /&gt;
&lt;br /&gt;
== References  ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; P. Atkins, J. De Paula, (n.d.). Physical chemistry. 7th edition.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics Prentice-Hall.&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794108</id>
		<title>MRD:Jsr3217</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794108"/>
		<updated>2019-06-03T14:34:31Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Question 4: 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 tab...&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System  ==&lt;br /&gt;
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If we define H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; as A and BC in our system, as the hydrogen atom collides with the hydrogen molecule, provided H has enough momentum and thus enough energy, the system changes and is described as AB and C where AB is our new diatomic product (A,B and C are the same type of atom).  &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;
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The transition state for this triatomic collision is a saddle point located at the intersection of the two potential energy surfaces, one PES for the Hydrogen atom and 1 PES for the Hydrogen molecule. The transition state is also a maximum on the trajectory pathway.&lt;br /&gt;
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Firstly the transition state being a turning point has a derivative of 0 with respect to q. This is shown by the following equation: (∂V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) and (∂V(q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)=0. However being a saddle point, the transition state is also defined as the point in the surface plot where there is a minimum in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction but also a maximum in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction, where q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are orthogonal to each other . This is where we have to take into account the second derivative of the potential energy V with respect to q. Mathematically these results are expressed as ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;gt;0 and ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;lt;0. The former second order differential equation refers to the minimum point in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction and the latter second order differential equation refers to the maximum point in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction.&lt;br /&gt;
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The transition state can be distinguished from a local minimum of the potential energy surface as by definition a local minimum will only have one 2nd derivative of potential energy (with respect to q in this case) which is greater than 0. However the transition state, being a saddle point, is a point with 2 second derivatives of potential energy in two different directions, one which is greater than 0 and one which is less than 0. &lt;br /&gt;
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{{fontcolor|pink|I can tell from this explanation that you understand the shape of the TS on the PES however your discussion here is not quite complete as you haven&#039;t defined the directions q1 and q2 so you haven&#039;t fully defined the shape of the TS. A diagram with the vectors included would be really helpful here. In general diagrams are useful! Also, the below statement about the equal distances is true of this system only because it is a special case where the system is symmetrical. Be careful using this statement as it is not a generic description of a TS.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:23, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Original Surface Plot showing both Potential Energy Surfaces and the Trajectory Pathway:&lt;br /&gt;
&lt;br /&gt;
[[File:1st surface plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the point where the interatomic distances are equal i.e. when the bond length of A-B is equal to the bond length of B-C. This is when the A-B bond is forming to make the diatomic product AB and the B-C bond is breaking leaving C on its own. This is shown below in the contour plot:&lt;br /&gt;
[[File:1st contour plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== Question 2: What is 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;
&lt;br /&gt;
The position of the transition state can be found by varying the AB and BC distances, with both momentum values of AB and BC being 0, until no variation in the Internuclear Distances vs Time Plot is noticed or until a straight line in the plot is seen. No variation or oscillation in the plot means there are no vibrations which is what happens in the transition state. The distance at which no oscillation was seen was found to be at 0.90774 Å.&lt;br /&gt;
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Internuclear Distance vs Time Plot at the transition state:&lt;br /&gt;
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[[File:2nd question graph 1.PNG]]&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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The plot with the MEP calculation shows a relatively short line with little variation in the y-axis (AB distance) however, the plot with the Dynamics calculation shows an oscillating line. The trajectory for the dynamics calculated plot is also longer in length than the MEP calculated plot. This is due to the MEP calculation not considering any vibrational modes therefore no oscillations are shown on the plot. In actuality, atoms have mass and momentum and so the vibrations of the hydrogen molecule are taken into account shown by the oscillations in the dynamics calculation plot. Thus the model with the dynamics calculation is the more accurate one.&lt;br /&gt;
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Plot with MEP Calculation:&lt;br /&gt;
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[[File:ACTUALMEP1.PNG]]&lt;br /&gt;
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Plot with Dynamics Calculation:&lt;br /&gt;
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[[File:ACTUALDYNAMIC.PNG]]&lt;br /&gt;
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{{fontcolor|pink|Your observations are valid, but can you think of why the MEP calculations shows no oscillations while the Dynamics calculation does, in terms of the calculation itself? An in depth understanding of the calculation process should aid in understanding the difference between the two methods. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:32, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 4: 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;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|+ Reactive or Unreactive Trajectories?&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the Trajectory !! Description &lt;br /&gt;
|-&lt;br /&gt;
| -1.25	|| -2.5	||-99.018 || Yes || [[File:1T.PNG]] ||Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products.|| &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.0	|| -100.456 || No || [[File:2T.PNG]] || Contour Plot shows that reaction does not occur as reactants don&#039;t have enough initial momentum and thus required (kinetic) energy to get over the activation energy barrier and reach the energy of the transition state. This is shown by the trajectory not reaching the transition state point and tailing back to the reactants. As the transition state isn&#039;t reached, the products aren&#039;t formed. || &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.5	|| -98.956|| Yes ||[[File:3T.PNG]] || Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products. The reaction is successful as the reactants have enough initial momentum and thus energy to reach the energy of the transition state. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.0	|| -84.956 || No || [[File:4T.PNG]] || Contour Plot shows although he reactants have enough initial momentum and thus energy to go through the transition state, the transition state collapses back into the reactants. This happens because of barrier recrossing. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.2	|| -83.416 || Yes || [[File:5T.PNG]] || Trajectory from contour plot shows that the reaction goes through/reaches the transition state point more than once. This occurs because of barrier recrossing again. However with these specific reaction conditions, the reaction does take place and the products are formed from the transition state. ||&lt;br /&gt;
|}&lt;br /&gt;
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&lt;br /&gt;
{{fontcolor|pink|What can you conclude overall from the table? Is the deciding factor in whether or not a reaction is successful as simple as a threshold activation energy, which if the molecules have they will definitely react?[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:34, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Question 5: State what are the main assumptions of Transition State Theory. 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;
&lt;br /&gt;
Transition State Theory assumes and tells us that states that &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; the transition state or activated complex in a reaction is in equilibrium with the reactants and once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. It also assumes the energy of the particles follows a Boltzmann distribution&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; but in this system since there are only 3 atoms in total for this triatomic collision there is no boltzmann distribution. As just mentioned, transition state theory assumes once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. However in contour plot 4 above where the trajectory shows that although the reaction goes through the transition state, the reactants are still reformed. This is because of barrier recrossing as mentioned above; with this present, the rate of this reaction, experimentally determined, would be lower than the reaction rate that the transition state theory would predict.&lt;br /&gt;
&lt;br /&gt;
== F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
=== Question 1: 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;br /&gt;
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&lt;br /&gt;
[[File:D1.PNG]]&lt;br /&gt;
&lt;br /&gt;
The above surface plot shows the potential energy surface for the exothermic conversion of F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to HF and H. The potential energy well slopes downwards from the reactants to the products showing that the energy of the products is lower than the energy of reactants. This reaction is an exothermic one as the bond strength of HF, the product, is stronger than the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactant. This means that the energy released from the formation of the HF bond is greater than the energy required to break the H-H bond in the hydrogen reactant molecule making the overall reaction exothermic.&lt;br /&gt;
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[[File:D2endo.PNG]]&lt;br /&gt;
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The above surface plot shows the potential energy surface for the endothermic conversion of HF and H to H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F. This reaction is the reverse reaction of the exothermic conversion we&#039;ve just considered. This potenital energy well slopes upwards from the reactants to the products showing that the energy of the products is higher than the energy of reactants making the reaction endothermic. The energy released from the hydrogen molecule, the product, is less than the energy taken in to break in the H-F bond in the reactant making the overall reaction endothermic.&lt;br /&gt;
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=== Question 2: Locate the approximate position of the transition state. ===&lt;br /&gt;
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Hammond&#039;s postulate essentially states that if 2 species are of similar energy they are of a similar structure. Thus in this reaction we can deduce that the transition state will be similar in structure to the reactants of the forward exothermic reaction, F and H2. By testing and varying the bond distances of F-H and H-H until the forces exterted on each other were 0 (characteristic in the transition state) the internuclear distances found were 1.811 Å for F-H and 0.745 for H-H Å.&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 easily calculated by taking away the reactant energy from the transition state energy. Using the internuclear distances of the atoms in the transition state calculated above in the settings function in the programme, the energy of the transition state was found to be -103.752 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;. The energy of the reactants, for the exothermic reaction for example, was found by inputting the normal bond length for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and making the distance between F and H relatively large so they&#039;re not interacting yielding the lowest energy for the reactants possible. From this the activation energies for the exothermic reaction was found to be 30.267 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; and the activation energy for the endothermic reaction was found to be 0.242 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;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 for the reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
&lt;br /&gt;
Due to the conservation of energy, all initial kinetic energy from the reactants&#039; momentum is converted and released as heat in the reaction once the products HF and H are formed. Due to the release of heat the surroundings temperature would increase as this is an exothermic reaction. This temperature change or increase in this case can be recorded by bomb calorimetry.&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 for the reaction HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
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For this endothermic reaction (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) there are two main modes of reactant energy to consider as the reactants approach the energy barrier/transition state point to form the products; these modes of energy are translational and vibrational energy. &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;Polanyi stated that for simple reactions described as an A + BC system, such as this H + HF system, if they have a late transition state, reactants with high vibrational energy is more effective for the reaction and its success, than reactants with high translational energy. This is because for a late transition state reaction, reactant molecules with high vibrational energy, if in the correct orientation, can vibrate their way to the top of the barrier, passing through the transition state forming the products successfully; however, if the reactants had high translational energy, in trying to reach the top of the energy barrier, they would just collide into the inner wall of the potential energy well and return to where they came from. This reaction being considered here (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) is an endothermic reaction with a late transition state as shown by the surface plot discussed earlier. Therefore to maximise the efficiency and the success of this reaction, reactants should have high vibrational energy. Polanyi also implied, that in this type of reaction (endothermic and late transition state), the products are likely to have high translational energy if the reaction effectively occurs with high vibrational energy reactants.&lt;br /&gt;
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The reaction showing highest efficiency and most effectiveness for its success was then modelled; high vibrational energy was inputted in the settings function for the molecule HF and high initial momentum of the incoming hydrogen atom for the collision was also inputted. However, unfortunately no such combination of momenta and bond length values were found that yielded a successful reaction, but below shows a contour plot with high vibrational energy in the reactants as shown by the oscillating trajectory which is what is needed to ensure high efficiency of this late transition state endothermic reaction.&lt;br /&gt;
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[[File:Loooool.png]]&lt;br /&gt;
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== References  ==&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; P. Atkins, J. De Paula, (n.d.). Physical chemistry. 7th edition.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics Prentice-Hall.&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794107</id>
		<title>MRD:Jsr3217</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794107"/>
		<updated>2019-06-03T14:32:29Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Question 3: Comment on how the MEP and the trajectory you just calculated differ. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System  ==&lt;br /&gt;
&lt;br /&gt;
If we define H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; as A and BC in our system, as the hydrogen atom collides with the hydrogen molecule, provided H has enough momentum and thus enough energy, the system changes and is described as AB and C where AB is our new diatomic product (A,B and C are the same type of atom).  &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;
&lt;br /&gt;
The transition state for this triatomic collision is a saddle point located at the intersection of the two potential energy surfaces, one PES for the Hydrogen atom and 1 PES for the Hydrogen molecule. The transition state is also a maximum on the trajectory pathway.&lt;br /&gt;
&lt;br /&gt;
Firstly the transition state being a turning point has a derivative of 0 with respect to q. This is shown by the following equation: (∂V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) and (∂V(q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)=0. However being a saddle point, the transition state is also defined as the point in the surface plot where there is a minimum in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction but also a maximum in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction, where q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are orthogonal to each other . This is where we have to take into account the second derivative of the potential energy V with respect to q. Mathematically these results are expressed as ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;gt;0 and ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;lt;0. The former second order differential equation refers to the minimum point in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction and the latter second order differential equation refers to the maximum point in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction.&lt;br /&gt;
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The transition state can be distinguished from a local minimum of the potential energy surface as by definition a local minimum will only have one 2nd derivative of potential energy (with respect to q in this case) which is greater than 0. However the transition state, being a saddle point, is a point with 2 second derivatives of potential energy in two different directions, one which is greater than 0 and one which is less than 0. &lt;br /&gt;
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{{fontcolor|pink|I can tell from this explanation that you understand the shape of the TS on the PES however your discussion here is not quite complete as you haven&#039;t defined the directions q1 and q2 so you haven&#039;t fully defined the shape of the TS. A diagram with the vectors included would be really helpful here. In general diagrams are useful! Also, the below statement about the equal distances is true of this system only because it is a special case where the system is symmetrical. Be careful using this statement as it is not a generic description of a TS.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:23, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Original Surface Plot showing both Potential Energy Surfaces and the Trajectory Pathway:&lt;br /&gt;
&lt;br /&gt;
[[File:1st surface plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the point where the interatomic distances are equal i.e. when the bond length of A-B is equal to the bond length of B-C. This is when the A-B bond is forming to make the diatomic product AB and the B-C bond is breaking leaving C on its own. This is shown below in the contour plot:&lt;br /&gt;
[[File:1st contour plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== Question 2: What is 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;
&lt;br /&gt;
The position of the transition state can be found by varying the AB and BC distances, with both momentum values of AB and BC being 0, until no variation in the Internuclear Distances vs Time Plot is noticed or until a straight line in the plot is seen. No variation or oscillation in the plot means there are no vibrations which is what happens in the transition state. The distance at which no oscillation was seen was found to be at 0.90774 Å.&lt;br /&gt;
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Internuclear Distance vs Time Plot at the transition state:&lt;br /&gt;
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[[File:2nd question graph 1.PNG]]&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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The plot with the MEP calculation shows a relatively short line with little variation in the y-axis (AB distance) however, the plot with the Dynamics calculation shows an oscillating line. The trajectory for the dynamics calculated plot is also longer in length than the MEP calculated plot. This is due to the MEP calculation not considering any vibrational modes therefore no oscillations are shown on the plot. In actuality, atoms have mass and momentum and so the vibrations of the hydrogen molecule are taken into account shown by the oscillations in the dynamics calculation plot. Thus the model with the dynamics calculation is the more accurate one.&lt;br /&gt;
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Plot with MEP Calculation:&lt;br /&gt;
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[[File:ACTUALMEP1.PNG]]&lt;br /&gt;
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Plot with Dynamics Calculation:&lt;br /&gt;
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[[File:ACTUALDYNAMIC.PNG]]&lt;br /&gt;
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{{fontcolor|pink|Your observations are valid, but can you think of why the MEP calculations shows no oscillations while the Dynamics calculation does, in terms of the calculation itself? An in depth understanding of the calculation process should aid in understanding the difference between the two methods. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:32, 3 June 2019 (BST)}}&lt;br /&gt;
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=== Question 4: 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;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|+ Reactive or Unreactive Trajectories?&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the Trajectory !! Description &lt;br /&gt;
|-&lt;br /&gt;
| -1.25	|| -2.5	||-99.018 || Yes || [[File:1T.PNG]] ||Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products.|| &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.0	|| -100.456 || No || [[File:2T.PNG]] || Contour Plot shows that reaction does not occur as reactants don&#039;t have enough initial momentum and thus required (kinetic) energy to get over the activation energy barrier and reach the energy of the transition state. This is shown by the trajectory not reaching the transition state point and tailing back to the reactants. As the transition state isn&#039;t reached, the products aren&#039;t formed. || &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.5	|| -98.956|| Yes ||[[File:3T.PNG]] || Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products. The reaction is successful as the reactants have enough initial momentum and thus energy to reach the energy of the transition state. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.0	|| -84.956 || No || [[File:4T.PNG]] || Contour Plot shows although he reactants have enough initial momentum and thus energy to go through the transition state, the transition state collapses back into the reactants. This happens because of barrier recrossing. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.2	|| -83.416 || Yes || [[File:5T.PNG]] || Trajectory from contour plot shows that the reaction goes through/reaches the transition state point more than once. This occurs because of barrier recrossing again. However with these specific reaction conditions, the reaction does take place and the products are formed from the transition state. ||&lt;br /&gt;
|}&lt;br /&gt;
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=== Question 5: State what are the main assumptions of Transition State Theory. 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 and tells us that states that &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; the transition state or activated complex in a reaction is in equilibrium with the reactants and once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. It also assumes the energy of the particles follows a Boltzmann distribution&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; but in this system since there are only 3 atoms in total for this triatomic collision there is no boltzmann distribution. As just mentioned, transition state theory assumes once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. However in contour plot 4 above where the trajectory shows that although the reaction goes through the transition state, the reactants are still reformed. This is because of barrier recrossing as mentioned above; with this present, the rate of this reaction, experimentally determined, would be lower than the reaction rate that the transition state theory would predict.&lt;br /&gt;
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== F - H - H system ==&lt;br /&gt;
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=== Question 1: 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;br /&gt;
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[[File:D1.PNG]]&lt;br /&gt;
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The above surface plot shows the potential energy surface for the exothermic conversion of F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to HF and H. The potential energy well slopes downwards from the reactants to the products showing that the energy of the products is lower than the energy of reactants. This reaction is an exothermic one as the bond strength of HF, the product, is stronger than the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactant. This means that the energy released from the formation of the HF bond is greater than the energy required to break the H-H bond in the hydrogen reactant molecule making the overall reaction exothermic.&lt;br /&gt;
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[[File:D2endo.PNG]]&lt;br /&gt;
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The above surface plot shows the potential energy surface for the endothermic conversion of HF and H to H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F. This reaction is the reverse reaction of the exothermic conversion we&#039;ve just considered. This potenital energy well slopes upwards from the reactants to the products showing that the energy of the products is higher than the energy of reactants making the reaction endothermic. The energy released from the hydrogen molecule, the product, is less than the energy taken in to break in the H-F bond in the reactant making the overall reaction endothermic.&lt;br /&gt;
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=== Question 2: Locate the approximate position of the transition state. ===&lt;br /&gt;
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Hammond&#039;s postulate essentially states that if 2 species are of similar energy they are of a similar structure. Thus in this reaction we can deduce that the transition state will be similar in structure to the reactants of the forward exothermic reaction, F and H2. By testing and varying the bond distances of F-H and H-H until the forces exterted on each other were 0 (characteristic in the transition state) the internuclear distances found were 1.811 Å for F-H and 0.745 for H-H Å.&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 easily calculated by taking away the reactant energy from the transition state energy. Using the internuclear distances of the atoms in the transition state calculated above in the settings function in the programme, the energy of the transition state was found to be -103.752 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;. The energy of the reactants, for the exothermic reaction for example, was found by inputting the normal bond length for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and making the distance between F and H relatively large so they&#039;re not interacting yielding the lowest energy for the reactants possible. From this the activation energies for the exothermic reaction was found to be 30.267 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; and the activation energy for the endothermic reaction was found to be 0.242 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&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 for the reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
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Due to the conservation of energy, all initial kinetic energy from the reactants&#039; momentum is converted and released as heat in the reaction once the products HF and H are formed. Due to the release of heat the surroundings temperature would increase as this is an exothermic reaction. This temperature change or increase in this case can be recorded by bomb calorimetry.&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 for the reaction HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
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For this endothermic reaction (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) there are two main modes of reactant energy to consider as the reactants approach the energy barrier/transition state point to form the products; these modes of energy are translational and vibrational energy. &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;Polanyi stated that for simple reactions described as an A + BC system, such as this H + HF system, if they have a late transition state, reactants with high vibrational energy is more effective for the reaction and its success, than reactants with high translational energy. This is because for a late transition state reaction, reactant molecules with high vibrational energy, if in the correct orientation, can vibrate their way to the top of the barrier, passing through the transition state forming the products successfully; however, if the reactants had high translational energy, in trying to reach the top of the energy barrier, they would just collide into the inner wall of the potential energy well and return to where they came from. This reaction being considered here (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) is an endothermic reaction with a late transition state as shown by the surface plot discussed earlier. Therefore to maximise the efficiency and the success of this reaction, reactants should have high vibrational energy. Polanyi also implied, that in this type of reaction (endothermic and late transition state), the products are likely to have high translational energy if the reaction effectively occurs with high vibrational energy reactants.&lt;br /&gt;
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The reaction showing highest efficiency and most effectiveness for its success was then modelled; high vibrational energy was inputted in the settings function for the molecule HF and high initial momentum of the incoming hydrogen atom for the collision was also inputted. However, unfortunately no such combination of momenta and bond length values were found that yielded a successful reaction, but below shows a contour plot with high vibrational energy in the reactants as shown by the oscillating trajectory which is what is needed to ensure high efficiency of this late transition state endothermic reaction.&lt;br /&gt;
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[[File:Loooool.png]]&lt;br /&gt;
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== References  ==&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; P. Atkins, J. De Paula, (n.d.). Physical chemistry. 7th edition.&lt;br /&gt;
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&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics Prentice-Hall.&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794106</id>
		<title>MRD:Jsr3217</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794106"/>
		<updated>2019-06-03T14:28:59Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* 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;== H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System  ==&lt;br /&gt;
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If we define H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; as A and BC in our system, as the hydrogen atom collides with the hydrogen molecule, provided H has enough momentum and thus enough energy, the system changes and is described as AB and C where AB is our new diatomic product (A,B and C are the same type of atom).  &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;
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The transition state for this triatomic collision is a saddle point located at the intersection of the two potential energy surfaces, one PES for the Hydrogen atom and 1 PES for the Hydrogen molecule. The transition state is also a maximum on the trajectory pathway.&lt;br /&gt;
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Firstly the transition state being a turning point has a derivative of 0 with respect to q. This is shown by the following equation: (∂V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) and (∂V(q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)=0. However being a saddle point, the transition state is also defined as the point in the surface plot where there is a minimum in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction but also a maximum in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction, where q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are orthogonal to each other . This is where we have to take into account the second derivative of the potential energy V with respect to q. Mathematically these results are expressed as ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;gt;0 and ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;lt;0. The former second order differential equation refers to the minimum point in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction and the latter second order differential equation refers to the maximum point in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction.&lt;br /&gt;
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The transition state can be distinguished from a local minimum of the potential energy surface as by definition a local minimum will only have one 2nd derivative of potential energy (with respect to q in this case) which is greater than 0. However the transition state, being a saddle point, is a point with 2 second derivatives of potential energy in two different directions, one which is greater than 0 and one which is less than 0. &lt;br /&gt;
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{{fontcolor|pink|I can tell from this explanation that you understand the shape of the TS on the PES however your discussion here is not quite complete as you haven&#039;t defined the directions q1 and q2 so you haven&#039;t fully defined the shape of the TS. A diagram with the vectors included would be really helpful here. In general diagrams are useful! Also, the below statement about the equal distances is true of this system only because it is a special case where the system is symmetrical. Be careful using this statement as it is not a generic description of a TS.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:23, 3 June 2019 (BST)}}&lt;br /&gt;
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Original Surface Plot showing both Potential Energy Surfaces and the Trajectory Pathway:&lt;br /&gt;
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[[File:1st surface plot.PNG]]&lt;br /&gt;
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The transition state is located at the point where the interatomic distances are equal i.e. when the bond length of A-B is equal to the bond length of B-C. This is when the A-B bond is forming to make the diatomic product AB and the B-C bond is breaking leaving C on its own. This is shown below in the contour plot:&lt;br /&gt;
[[File:1st contour plot.PNG]]&lt;br /&gt;
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=== Question 2: What is 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;
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The position of the transition state can be found by varying the AB and BC distances, with both momentum values of AB and BC being 0, until no variation in the Internuclear Distances vs Time Plot is noticed or until a straight line in the plot is seen. No variation or oscillation in the plot means there are no vibrations which is what happens in the transition state. The distance at which no oscillation was seen was found to be at 0.90774 Å.&lt;br /&gt;
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Internuclear Distance vs Time Plot at the transition state:&lt;br /&gt;
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[[File:2nd question graph 1.PNG]]&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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The plot with the MEP calculation shows a relatively short line with little variation in the y-axis (AB distance) however, the plot with the Dynamics calculation shows an oscillating line. The trajectory for the dynamics calculated plot is also longer in length than the MEP calculated plot. This is due to the MEP calculation not considering any vibrational modes therefore no oscillations are shown on the plot. In actuality, atoms have mass and momentum and so the vibrations of the hydrogen molecule are taken into account shown by the oscillations in the dynamics calculation plot. Thus the model with the dynamics calculation is the more accurate one.&lt;br /&gt;
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Plot with MEP Calculation:&lt;br /&gt;
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[[File:ACTUALMEP1.PNG]]&lt;br /&gt;
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Plot with Dynamics Calculation:&lt;br /&gt;
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[[File:ACTUALDYNAMIC.PNG]]&lt;br /&gt;
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=== Question 4: 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;
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{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|+ Reactive or Unreactive Trajectories?&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the Trajectory !! Description &lt;br /&gt;
|-&lt;br /&gt;
| -1.25	|| -2.5	||-99.018 || Yes || [[File:1T.PNG]] ||Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products.|| &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.0	|| -100.456 || No || [[File:2T.PNG]] || Contour Plot shows that reaction does not occur as reactants don&#039;t have enough initial momentum and thus required (kinetic) energy to get over the activation energy barrier and reach the energy of the transition state. This is shown by the trajectory not reaching the transition state point and tailing back to the reactants. As the transition state isn&#039;t reached, the products aren&#039;t formed. || &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.5	|| -98.956|| Yes ||[[File:3T.PNG]] || Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products. The reaction is successful as the reactants have enough initial momentum and thus energy to reach the energy of the transition state. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.0	|| -84.956 || No || [[File:4T.PNG]] || Contour Plot shows although he reactants have enough initial momentum and thus energy to go through the transition state, the transition state collapses back into the reactants. This happens because of barrier recrossing. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.2	|| -83.416 || Yes || [[File:5T.PNG]] || Trajectory from contour plot shows that the reaction goes through/reaches the transition state point more than once. This occurs because of barrier recrossing again. However with these specific reaction conditions, the reaction does take place and the products are formed from the transition state. ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Question 5: State what are the main assumptions of Transition State Theory. 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 and tells us that states that &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; the transition state or activated complex in a reaction is in equilibrium with the reactants and once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. It also assumes the energy of the particles follows a Boltzmann distribution&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; but in this system since there are only 3 atoms in total for this triatomic collision there is no boltzmann distribution. As just mentioned, transition state theory assumes once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. However in contour plot 4 above where the trajectory shows that although the reaction goes through the transition state, the reactants are still reformed. This is because of barrier recrossing as mentioned above; with this present, the rate of this reaction, experimentally determined, would be lower than the reaction rate that the transition state theory would predict.&lt;br /&gt;
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== F - H - H system ==&lt;br /&gt;
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=== Question 1: 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;br /&gt;
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[[File:D1.PNG]]&lt;br /&gt;
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The above surface plot shows the potential energy surface for the exothermic conversion of F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to HF and H. The potential energy well slopes downwards from the reactants to the products showing that the energy of the products is lower than the energy of reactants. This reaction is an exothermic one as the bond strength of HF, the product, is stronger than the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactant. This means that the energy released from the formation of the HF bond is greater than the energy required to break the H-H bond in the hydrogen reactant molecule making the overall reaction exothermic.&lt;br /&gt;
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[[File:D2endo.PNG]]&lt;br /&gt;
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The above surface plot shows the potential energy surface for the endothermic conversion of HF and H to H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F. This reaction is the reverse reaction of the exothermic conversion we&#039;ve just considered. This potenital energy well slopes upwards from the reactants to the products showing that the energy of the products is higher than the energy of reactants making the reaction endothermic. The energy released from the hydrogen molecule, the product, is less than the energy taken in to break in the H-F bond in the reactant making the overall reaction endothermic.&lt;br /&gt;
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=== Question 2: Locate the approximate position of the transition state. ===&lt;br /&gt;
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Hammond&#039;s postulate essentially states that if 2 species are of similar energy they are of a similar structure. Thus in this reaction we can deduce that the transition state will be similar in structure to the reactants of the forward exothermic reaction, F and H2. By testing and varying the bond distances of F-H and H-H until the forces exterted on each other were 0 (characteristic in the transition state) the internuclear distances found were 1.811 Å for F-H and 0.745 for H-H Å.&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 easily calculated by taking away the reactant energy from the transition state energy. Using the internuclear distances of the atoms in the transition state calculated above in the settings function in the programme, the energy of the transition state was found to be -103.752 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;. The energy of the reactants, for the exothermic reaction for example, was found by inputting the normal bond length for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and making the distance between F and H relatively large so they&#039;re not interacting yielding the lowest energy for the reactants possible. From this the activation energies for the exothermic reaction was found to be 30.267 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; and the activation energy for the endothermic reaction was found to be 0.242 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&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 for the reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
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Due to the conservation of energy, all initial kinetic energy from the reactants&#039; momentum is converted and released as heat in the reaction once the products HF and H are formed. Due to the release of heat the surroundings temperature would increase as this is an exothermic reaction. This temperature change or increase in this case can be recorded by bomb calorimetry.&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 for the reaction HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For this endothermic reaction (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) there are two main modes of reactant energy to consider as the reactants approach the energy barrier/transition state point to form the products; these modes of energy are translational and vibrational energy. &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;Polanyi stated that for simple reactions described as an A + BC system, such as this H + HF system, if they have a late transition state, reactants with high vibrational energy is more effective for the reaction and its success, than reactants with high translational energy. This is because for a late transition state reaction, reactant molecules with high vibrational energy, if in the correct orientation, can vibrate their way to the top of the barrier, passing through the transition state forming the products successfully; however, if the reactants had high translational energy, in trying to reach the top of the energy barrier, they would just collide into the inner wall of the potential energy well and return to where they came from. This reaction being considered here (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) is an endothermic reaction with a late transition state as shown by the surface plot discussed earlier. Therefore to maximise the efficiency and the success of this reaction, reactants should have high vibrational energy. Polanyi also implied, that in this type of reaction (endothermic and late transition state), the products are likely to have high translational energy if the reaction effectively occurs with high vibrational energy reactants.&lt;br /&gt;
&lt;br /&gt;
The reaction showing highest efficiency and most effectiveness for its success was then modelled; high vibrational energy was inputted in the settings function for the molecule HF and high initial momentum of the incoming hydrogen atom for the collision was also inputted. However, unfortunately no such combination of momenta and bond length values were found that yielded a successful reaction, but below shows a contour plot with high vibrational energy in the reactants as shown by the oscillating trajectory which is what is needed to ensure high efficiency of this late transition state endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Loooool.png]]&lt;br /&gt;
&lt;br /&gt;
== References  ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; P. Atkins, J. De Paula, (n.d.). Physical chemistry. 7th edition.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics Prentice-Hall.&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794105</id>
		<title>MRD:Jsr3217</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794105"/>
		<updated>2019-06-03T14:28:29Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* 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;== H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System  ==&lt;br /&gt;
&lt;br /&gt;
If we define H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; as A and BC in our system, as the hydrogen atom collides with the hydrogen molecule, provided H has enough momentum and thus enough energy, the system changes and is described as AB and C where AB is our new diatomic product (A,B and C are the same type of atom).  &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;
&lt;br /&gt;
The transition state for this triatomic collision is a saddle point located at the intersection of the two potential energy surfaces, one PES for the Hydrogen atom and 1 PES for the Hydrogen molecule. The transition state is also a maximum on the trajectory pathway.&lt;br /&gt;
&lt;br /&gt;
Firstly the transition state being a turning point has a derivative of 0 with respect to q. This is shown by the following equation: (∂V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) and (∂V(q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)=0. However being a saddle point, the transition state is also defined as the point in the surface plot where there is a minimum in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction but also a maximum in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction, where q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are orthogonal to each other . This is where we have to take into account the second derivative of the potential energy V with respect to q. Mathematically these results are expressed as ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;gt;0 and ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;lt;0. The former second order differential equation refers to the minimum point in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction and the latter second order differential equation refers to the maximum point in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction.&lt;br /&gt;
&lt;br /&gt;
The transition state can be distinguished from a local minimum of the potential energy surface as by definition a local minimum will only have one 2nd derivative of potential energy (with respect to q in this case) which is greater than 0. However the transition state, being a saddle point, is a point with 2 second derivatives of potential energy in two different directions, one which is greater than 0 and one which is less than 0. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|I can tell from this explanation that you understand the shape of the TS on the PES however your discussion here is not quite complete as you haven&#039;t defined the directions q1 and q2 so you haven&#039;t fully defined the shape of the TS. A diagram with the vectors included would be really helpful here. In general diagrams are useful! Also, the below statement about the equal distances is true of this system only because it is a special case where A=B=C. Be careful using this statement as it is not a generic description of a TS.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:23, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Original Surface Plot showing both Potential Energy Surfaces and the Trajectory Pathway:&lt;br /&gt;
&lt;br /&gt;
[[File:1st surface plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the point where the interatomic distances are equal i.e. when the bond length of A-B is equal to the bond length of B-C. This is when the A-B bond is forming to make the diatomic product AB and the B-C bond is breaking leaving C on its own. This is shown below in the contour plot:&lt;br /&gt;
[[File:1st contour plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== Question 2: What is 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;
&lt;br /&gt;
The position of the transition state can be found by varying the AB and BC distances, with both momentum values of AB and BC being 0, until no variation in the Internuclear Distances vs Time Plot is noticed or until a straight line in the plot is seen. No variation or oscillation in the plot means there are no vibrations which is what happens in the transition state. The distance at which no oscillation was seen was found to be at 0.90774 Å.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Internuclear Distance vs Time Plot at the transition state:&lt;br /&gt;
&lt;br /&gt;
[[File:2nd question graph 1.PNG]]&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;
&lt;br /&gt;
&lt;br /&gt;
The plot with the MEP calculation shows a relatively short line with little variation in the y-axis (AB distance) however, the plot with the Dynamics calculation shows an oscillating line. The trajectory for the dynamics calculated plot is also longer in length than the MEP calculated plot. This is due to the MEP calculation not considering any vibrational modes therefore no oscillations are shown on the plot. In actuality, atoms have mass and momentum and so the vibrations of the hydrogen molecule are taken into account shown by the oscillations in the dynamics calculation plot. Thus the model with the dynamics calculation is the more accurate one.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Plot with MEP Calculation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ACTUALMEP1.PNG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Plot with Dynamics Calculation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ACTUALDYNAMIC.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== Question 4: 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;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|+ Reactive or Unreactive Trajectories?&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the Trajectory !! Description &lt;br /&gt;
|-&lt;br /&gt;
| -1.25	|| -2.5	||-99.018 || Yes || [[File:1T.PNG]] ||Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products.|| &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.0	|| -100.456 || No || [[File:2T.PNG]] || Contour Plot shows that reaction does not occur as reactants don&#039;t have enough initial momentum and thus required (kinetic) energy to get over the activation energy barrier and reach the energy of the transition state. This is shown by the trajectory not reaching the transition state point and tailing back to the reactants. As the transition state isn&#039;t reached, the products aren&#039;t formed. || &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.5	|| -98.956|| Yes ||[[File:3T.PNG]] || Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products. The reaction is successful as the reactants have enough initial momentum and thus energy to reach the energy of the transition state. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.0	|| -84.956 || No || [[File:4T.PNG]] || Contour Plot shows although he reactants have enough initial momentum and thus energy to go through the transition state, the transition state collapses back into the reactants. This happens because of barrier recrossing. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.2	|| -83.416 || Yes || [[File:5T.PNG]] || Trajectory from contour plot shows that the reaction goes through/reaches the transition state point more than once. This occurs because of barrier recrossing again. However with these specific reaction conditions, the reaction does take place and the products are formed from the transition state. ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Question 5: State what are the main assumptions of Transition State Theory. 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;
&lt;br /&gt;
Transition State Theory assumes and tells us that states that &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; the transition state or activated complex in a reaction is in equilibrium with the reactants and once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. It also assumes the energy of the particles follows a Boltzmann distribution&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; but in this system since there are only 3 atoms in total for this triatomic collision there is no boltzmann distribution. As just mentioned, transition state theory assumes once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. However in contour plot 4 above where the trajectory shows that although the reaction goes through the transition state, the reactants are still reformed. This is because of barrier recrossing as mentioned above; with this present, the rate of this reaction, experimentally determined, would be lower than the reaction rate that the transition state theory would predict.&lt;br /&gt;
&lt;br /&gt;
== F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
=== Question 1: 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;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:D1.PNG]]&lt;br /&gt;
&lt;br /&gt;
The above surface plot shows the potential energy surface for the exothermic conversion of F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to HF and H. The potential energy well slopes downwards from the reactants to the products showing that the energy of the products is lower than the energy of reactants. This reaction is an exothermic one as the bond strength of HF, the product, is stronger than the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactant. This means that the energy released from the formation of the HF bond is greater than the energy required to break the H-H bond in the hydrogen reactant molecule making the overall reaction exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:D2endo.PNG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The above surface plot shows the potential energy surface for the endothermic conversion of HF and H to H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F. This reaction is the reverse reaction of the exothermic conversion we&#039;ve just considered. This potenital energy well slopes upwards from the reactants to the products showing that the energy of the products is higher than the energy of reactants making the reaction endothermic. The energy released from the hydrogen molecule, the product, is less than the energy taken in to break in the H-F bond in the reactant making the overall reaction endothermic.&lt;br /&gt;
&lt;br /&gt;
=== Question 2: Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate essentially states that if 2 species are of similar energy they are of a similar structure. Thus in this reaction we can deduce that the transition state will be similar in structure to the reactants of the forward exothermic reaction, F and H2. By testing and varying the bond distances of F-H and H-H until the forces exterted on each other were 0 (characteristic in the transition state) the internuclear distances found were 1.811 Å for F-H and 0.745 for H-H Å.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Question 3: Report the activation energy for both reactions. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The activation energy can be easily calculated by taking away the reactant energy from the transition state energy. Using the internuclear distances of the atoms in the transition state calculated above in the settings function in the programme, the energy of the transition state was found to be -103.752 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;. The energy of the reactants, for the exothermic reaction for example, was found by inputting the normal bond length for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and making the distance between F and H relatively large so they&#039;re not interacting yielding the lowest energy for the reactants possible. From this the activation energies for the exothermic reaction was found to be 30.267 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; and the activation energy for the endothermic reaction was found to be 0.242 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;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 for the reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
&lt;br /&gt;
Due to the conservation of energy, all initial kinetic energy from the reactants&#039; momentum is converted and released as heat in the reaction once the products HF and H are formed. Due to the release of heat the surroundings temperature would increase as this is an exothermic reaction. This temperature change or increase in this case can be recorded by bomb calorimetry.&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 for the reaction HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For this endothermic reaction (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) there are two main modes of reactant energy to consider as the reactants approach the energy barrier/transition state point to form the products; these modes of energy are translational and vibrational energy. &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;Polanyi stated that for simple reactions described as an A + BC system, such as this H + HF system, if they have a late transition state, reactants with high vibrational energy is more effective for the reaction and its success, than reactants with high translational energy. This is because for a late transition state reaction, reactant molecules with high vibrational energy, if in the correct orientation, can vibrate their way to the top of the barrier, passing through the transition state forming the products successfully; however, if the reactants had high translational energy, in trying to reach the top of the energy barrier, they would just collide into the inner wall of the potential energy well and return to where they came from. This reaction being considered here (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) is an endothermic reaction with a late transition state as shown by the surface plot discussed earlier. Therefore to maximise the efficiency and the success of this reaction, reactants should have high vibrational energy. Polanyi also implied, that in this type of reaction (endothermic and late transition state), the products are likely to have high translational energy if the reaction effectively occurs with high vibrational energy reactants.&lt;br /&gt;
&lt;br /&gt;
The reaction showing highest efficiency and most effectiveness for its success was then modelled; high vibrational energy was inputted in the settings function for the molecule HF and high initial momentum of the incoming hydrogen atom for the collision was also inputted. However, unfortunately no such combination of momenta and bond length values were found that yielded a successful reaction, but below shows a contour plot with high vibrational energy in the reactants as shown by the oscillating trajectory which is what is needed to ensure high efficiency of this late transition state endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Loooool.png]]&lt;br /&gt;
&lt;br /&gt;
== References  ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; P. Atkins, J. De Paula, (n.d.). Physical chemistry. 7th edition.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics Prentice-Hall.&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794104</id>
		<title>MRD:Jsr3217</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794104"/>
		<updated>2019-06-03T14:27:47Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* 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;== H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System  ==&lt;br /&gt;
&lt;br /&gt;
If we define H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; as A and BC in our system, as the hydrogen atom collides with the hydrogen molecule, provided H has enough momentum and thus enough energy, the system changes and is described as AB and C where AB is our new diatomic product (A,B and C are the same type of atom).  &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;
&lt;br /&gt;
The transition state for this triatomic collision is a saddle point located at the intersection of the two potential energy surfaces, one PES for the Hydrogen atom and 1 PES for the Hydrogen molecule. The transition state is also a maximum on the trajectory pathway.&lt;br /&gt;
&lt;br /&gt;
Firstly the transition state being a turning point has a derivative of 0 with respect to q. This is shown by the following equation: (∂V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) and (∂V(q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)=0. However being a saddle point, the transition state is also defined as the point in the surface plot where there is a minimum in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction but also a maximum in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction, where q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are orthogonal to each other . This is where we have to take into account the second derivative of the potential energy V with respect to q. Mathematically these results are expressed as ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;gt;0 and ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;lt;0. The former second order differential equation refers to the minimum point in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction and the latter second order differential equation refers to the maximum point in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction.&lt;br /&gt;
&lt;br /&gt;
The transition state can be distinguished from a local minimum of the potential energy surface as by definition a local minimum will only have one 2nd derivative of potential energy (with respect to q in this case) which is greater than 0. However the transition state, being a saddle point, is a point with 2 second derivatives of potential energy in two different directions, one which is greater than 0 and one which is less than 0. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|I can tell from this explanation that you understand the shape of the TS on the PES however your discussion here is not quite complete as you haven&#039;t defined the directions q1 and q2 so you haven&#039;t fully defined the shape of the TS. A diagram with the vectors included would be really helpful here. In general diagrams are useful! [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:23, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Original Surface Plot showing both Potential Energy Surfaces and the Trajectory Pathway:&lt;br /&gt;
&lt;br /&gt;
[[File:1st surface plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the point where the interatomic distances are equal i.e. when the bond length of A-B is equal to the bond length of B-C. This is when the A-B bond is forming to make the diatomic product AB and the B-C bond is breaking leaving C on its own. This is shown below in the contour plot:&lt;br /&gt;
{{fontcolor|pink|This statement about the equal distances is true of this system only because it is a special case where A=B=C. Be careful using this statement as it is not a generic description of a TS.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:27, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
[[File:1st contour plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== Question 2: What is 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;
&lt;br /&gt;
The position of the transition state can be found by varying the AB and BC distances, with both momentum values of AB and BC being 0, until no variation in the Internuclear Distances vs Time Plot is noticed or until a straight line in the plot is seen. No variation or oscillation in the plot means there are no vibrations which is what happens in the transition state. The distance at which no oscillation was seen was found to be at 0.90774 Å.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Internuclear Distance vs Time Plot at the transition state:&lt;br /&gt;
&lt;br /&gt;
[[File:2nd question graph 1.PNG]]&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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The plot with the MEP calculation shows a relatively short line with little variation in the y-axis (AB distance) however, the plot with the Dynamics calculation shows an oscillating line. The trajectory for the dynamics calculated plot is also longer in length than the MEP calculated plot. This is due to the MEP calculation not considering any vibrational modes therefore no oscillations are shown on the plot. In actuality, atoms have mass and momentum and so the vibrations of the hydrogen molecule are taken into account shown by the oscillations in the dynamics calculation plot. Thus the model with the dynamics calculation is the more accurate one.&lt;br /&gt;
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Plot with MEP Calculation:&lt;br /&gt;
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[[File:ACTUALMEP1.PNG]]&lt;br /&gt;
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Plot with Dynamics Calculation:&lt;br /&gt;
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[[File:ACTUALDYNAMIC.PNG]]&lt;br /&gt;
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=== Question 4: 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;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|+ Reactive or Unreactive Trajectories?&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the Trajectory !! Description &lt;br /&gt;
|-&lt;br /&gt;
| -1.25	|| -2.5	||-99.018 || Yes || [[File:1T.PNG]] ||Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products.|| &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.0	|| -100.456 || No || [[File:2T.PNG]] || Contour Plot shows that reaction does not occur as reactants don&#039;t have enough initial momentum and thus required (kinetic) energy to get over the activation energy barrier and reach the energy of the transition state. This is shown by the trajectory not reaching the transition state point and tailing back to the reactants. As the transition state isn&#039;t reached, the products aren&#039;t formed. || &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.5	|| -98.956|| Yes ||[[File:3T.PNG]] || Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products. The reaction is successful as the reactants have enough initial momentum and thus energy to reach the energy of the transition state. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.0	|| -84.956 || No || [[File:4T.PNG]] || Contour Plot shows although he reactants have enough initial momentum and thus energy to go through the transition state, the transition state collapses back into the reactants. This happens because of barrier recrossing. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.2	|| -83.416 || Yes || [[File:5T.PNG]] || Trajectory from contour plot shows that the reaction goes through/reaches the transition state point more than once. This occurs because of barrier recrossing again. However with these specific reaction conditions, the reaction does take place and the products are formed from the transition state. ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Question 5: State what are the main assumptions of Transition State Theory. 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;
&lt;br /&gt;
Transition State Theory assumes and tells us that states that &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; the transition state or activated complex in a reaction is in equilibrium with the reactants and once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. It also assumes the energy of the particles follows a Boltzmann distribution&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; but in this system since there are only 3 atoms in total for this triatomic collision there is no boltzmann distribution. As just mentioned, transition state theory assumes once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. However in contour plot 4 above where the trajectory shows that although the reaction goes through the transition state, the reactants are still reformed. This is because of barrier recrossing as mentioned above; with this present, the rate of this reaction, experimentally determined, would be lower than the reaction rate that the transition state theory would predict.&lt;br /&gt;
&lt;br /&gt;
== F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
=== Question 1: 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;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:D1.PNG]]&lt;br /&gt;
&lt;br /&gt;
The above surface plot shows the potential energy surface for the exothermic conversion of F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to HF and H. The potential energy well slopes downwards from the reactants to the products showing that the energy of the products is lower than the energy of reactants. This reaction is an exothermic one as the bond strength of HF, the product, is stronger than the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactant. This means that the energy released from the formation of the HF bond is greater than the energy required to break the H-H bond in the hydrogen reactant molecule making the overall reaction exothermic.&lt;br /&gt;
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[[File:D2endo.PNG]]&lt;br /&gt;
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The above surface plot shows the potential energy surface for the endothermic conversion of HF and H to H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F. This reaction is the reverse reaction of the exothermic conversion we&#039;ve just considered. This potenital energy well slopes upwards from the reactants to the products showing that the energy of the products is higher than the energy of reactants making the reaction endothermic. The energy released from the hydrogen molecule, the product, is less than the energy taken in to break in the H-F bond in the reactant making the overall reaction endothermic.&lt;br /&gt;
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=== Question 2: Locate the approximate position of the transition state. ===&lt;br /&gt;
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Hammond&#039;s postulate essentially states that if 2 species are of similar energy they are of a similar structure. Thus in this reaction we can deduce that the transition state will be similar in structure to the reactants of the forward exothermic reaction, F and H2. By testing and varying the bond distances of F-H and H-H until the forces exterted on each other were 0 (characteristic in the transition state) the internuclear distances found were 1.811 Å for F-H and 0.745 for H-H Å.&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 easily calculated by taking away the reactant energy from the transition state energy. Using the internuclear distances of the atoms in the transition state calculated above in the settings function in the programme, the energy of the transition state was found to be -103.752 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;. The energy of the reactants, for the exothermic reaction for example, was found by inputting the normal bond length for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and making the distance between F and H relatively large so they&#039;re not interacting yielding the lowest energy for the reactants possible. From this the activation energies for the exothermic reaction was found to be 30.267 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; and the activation energy for the endothermic reaction was found to be 0.242 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;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 for the reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
&lt;br /&gt;
Due to the conservation of energy, all initial kinetic energy from the reactants&#039; momentum is converted and released as heat in the reaction once the products HF and H are formed. Due to the release of heat the surroundings temperature would increase as this is an exothermic reaction. This temperature change or increase in this case can be recorded by bomb calorimetry.&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 for the reaction HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
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For this endothermic reaction (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) there are two main modes of reactant energy to consider as the reactants approach the energy barrier/transition state point to form the products; these modes of energy are translational and vibrational energy. &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;Polanyi stated that for simple reactions described as an A + BC system, such as this H + HF system, if they have a late transition state, reactants with high vibrational energy is more effective for the reaction and its success, than reactants with high translational energy. This is because for a late transition state reaction, reactant molecules with high vibrational energy, if in the correct orientation, can vibrate their way to the top of the barrier, passing through the transition state forming the products successfully; however, if the reactants had high translational energy, in trying to reach the top of the energy barrier, they would just collide into the inner wall of the potential energy well and return to where they came from. This reaction being considered here (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) is an endothermic reaction with a late transition state as shown by the surface plot discussed earlier. Therefore to maximise the efficiency and the success of this reaction, reactants should have high vibrational energy. Polanyi also implied, that in this type of reaction (endothermic and late transition state), the products are likely to have high translational energy if the reaction effectively occurs with high vibrational energy reactants.&lt;br /&gt;
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The reaction showing highest efficiency and most effectiveness for its success was then modelled; high vibrational energy was inputted in the settings function for the molecule HF and high initial momentum of the incoming hydrogen atom for the collision was also inputted. However, unfortunately no such combination of momenta and bond length values were found that yielded a successful reaction, but below shows a contour plot with high vibrational energy in the reactants as shown by the oscillating trajectory which is what is needed to ensure high efficiency of this late transition state endothermic reaction.&lt;br /&gt;
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[[File:Loooool.png]]&lt;br /&gt;
&lt;br /&gt;
== References  ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; P. Atkins, J. De Paula, (n.d.). Physical chemistry. 7th edition.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics Prentice-Hall.&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794103</id>
		<title>MRD:Jsr3217</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794103"/>
		<updated>2019-06-03T14:26:56Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* 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;== H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System  ==&lt;br /&gt;
&lt;br /&gt;
If we define H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; as A and BC in our system, as the hydrogen atom collides with the hydrogen molecule, provided H has enough momentum and thus enough energy, the system changes and is described as AB and C where AB is our new diatomic product (A,B and C are the same type of atom).  &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;
&lt;br /&gt;
The transition state for this triatomic collision is a saddle point located at the intersection of the two potential energy surfaces, one PES for the Hydrogen atom and 1 PES for the Hydrogen molecule. The transition state is also a maximum on the trajectory pathway.&lt;br /&gt;
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Firstly the transition state being a turning point has a derivative of 0 with respect to q. This is shown by the following equation: (∂V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) and (∂V(q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)=0. However being a saddle point, the transition state is also defined as the point in the surface plot where there is a minimum in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction but also a maximum in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction, where q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are orthogonal to each other . This is where we have to take into account the second derivative of the potential energy V with respect to q. Mathematically these results are expressed as ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;gt;0 and ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;lt;0. The former second order differential equation refers to the minimum point in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction and the latter second order differential equation refers to the maximum point in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction.&lt;br /&gt;
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The transition state can be distinguished from a local minimum of the potential energy surface as by definition a local minimum will only have one 2nd derivative of potential energy (with respect to q in this case) which is greater than 0. However the transition state, being a saddle point, is a point with 2 second derivatives of potential energy in two different directions, one which is greater than 0 and one which is less than 0. &lt;br /&gt;
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{{fontcolor|pink|I can tell from this explanation that you understand the shape of the TS on the PES however your discussion here is not quite complete as you haven&#039;t defined the directions q1 and q2 so you haven&#039;t fully defined the shape of the TS. A diagram with the vectors included would be really helpful here. In general diagrams are useful! [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:23, 3 June 2019 (BST)}}&lt;br /&gt;
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Original Surface Plot showing both Potential Energy Surfaces and the Trajectory Pathway:&lt;br /&gt;
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[[File:1st surface plot.PNG]]&lt;br /&gt;
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The transition state is located at the point where the interatomic distances are equal i.e. when the bond length of A-B is equal to the bond length of B-C. This is when the A-B bond is forming to make the diatomic product AB and the B-C bond is breaking leaving C on its own. This is shown below in the contour plot:&lt;br /&gt;
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[[File:1st contour plot.PNG]]&lt;br /&gt;
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{{fontcolor|pink|This statement about the equal distances is true of this system only because it is a special case where A=B=C. Be careful using this statement as it is not a generic description of a TS. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:26, 3 June 2019 (BST)}}&lt;br /&gt;
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=== Question 2: What is 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;
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The position of the transition state can be found by varying the AB and BC distances, with both momentum values of AB and BC being 0, until no variation in the Internuclear Distances vs Time Plot is noticed or until a straight line in the plot is seen. No variation or oscillation in the plot means there are no vibrations which is what happens in the transition state. The distance at which no oscillation was seen was found to be at 0.90774 Å.&lt;br /&gt;
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Internuclear Distance vs Time Plot at the transition state:&lt;br /&gt;
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[[File:2nd question graph 1.PNG]]&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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The plot with the MEP calculation shows a relatively short line with little variation in the y-axis (AB distance) however, the plot with the Dynamics calculation shows an oscillating line. The trajectory for the dynamics calculated plot is also longer in length than the MEP calculated plot. This is due to the MEP calculation not considering any vibrational modes therefore no oscillations are shown on the plot. In actuality, atoms have mass and momentum and so the vibrations of the hydrogen molecule are taken into account shown by the oscillations in the dynamics calculation plot. Thus the model with the dynamics calculation is the more accurate one.&lt;br /&gt;
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Plot with MEP Calculation:&lt;br /&gt;
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[[File:ACTUALMEP1.PNG]]&lt;br /&gt;
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Plot with Dynamics Calculation:&lt;br /&gt;
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[[File:ACTUALDYNAMIC.PNG]]&lt;br /&gt;
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=== Question 4: 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;
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{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|+ Reactive or Unreactive Trajectories?&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the Trajectory !! Description &lt;br /&gt;
|-&lt;br /&gt;
| -1.25	|| -2.5	||-99.018 || Yes || [[File:1T.PNG]] ||Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products.|| &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.0	|| -100.456 || No || [[File:2T.PNG]] || Contour Plot shows that reaction does not occur as reactants don&#039;t have enough initial momentum and thus required (kinetic) energy to get over the activation energy barrier and reach the energy of the transition state. This is shown by the trajectory not reaching the transition state point and tailing back to the reactants. As the transition state isn&#039;t reached, the products aren&#039;t formed. || &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.5	|| -98.956|| Yes ||[[File:3T.PNG]] || Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products. The reaction is successful as the reactants have enough initial momentum and thus energy to reach the energy of the transition state. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.0	|| -84.956 || No || [[File:4T.PNG]] || Contour Plot shows although he reactants have enough initial momentum and thus energy to go through the transition state, the transition state collapses back into the reactants. This happens because of barrier recrossing. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.2	|| -83.416 || Yes || [[File:5T.PNG]] || Trajectory from contour plot shows that the reaction goes through/reaches the transition state point more than once. This occurs because of barrier recrossing again. However with these specific reaction conditions, the reaction does take place and the products are formed from the transition state. ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Question 5: State what are the main assumptions of Transition State Theory. 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 and tells us that states that &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; the transition state or activated complex in a reaction is in equilibrium with the reactants and once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. It also assumes the energy of the particles follows a Boltzmann distribution&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; but in this system since there are only 3 atoms in total for this triatomic collision there is no boltzmann distribution. As just mentioned, transition state theory assumes once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. However in contour plot 4 above where the trajectory shows that although the reaction goes through the transition state, the reactants are still reformed. This is because of barrier recrossing as mentioned above; with this present, the rate of this reaction, experimentally determined, would be lower than the reaction rate that the transition state theory would predict.&lt;br /&gt;
&lt;br /&gt;
== F - H - H system ==&lt;br /&gt;
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=== Question 1: 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;br /&gt;
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[[File:D1.PNG]]&lt;br /&gt;
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The above surface plot shows the potential energy surface for the exothermic conversion of F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to HF and H. The potential energy well slopes downwards from the reactants to the products showing that the energy of the products is lower than the energy of reactants. This reaction is an exothermic one as the bond strength of HF, the product, is stronger than the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactant. This means that the energy released from the formation of the HF bond is greater than the energy required to break the H-H bond in the hydrogen reactant molecule making the overall reaction exothermic.&lt;br /&gt;
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[[File:D2endo.PNG]]&lt;br /&gt;
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The above surface plot shows the potential energy surface for the endothermic conversion of HF and H to H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F. This reaction is the reverse reaction of the exothermic conversion we&#039;ve just considered. This potenital energy well slopes upwards from the reactants to the products showing that the energy of the products is higher than the energy of reactants making the reaction endothermic. The energy released from the hydrogen molecule, the product, is less than the energy taken in to break in the H-F bond in the reactant making the overall reaction endothermic.&lt;br /&gt;
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=== Question 2: Locate the approximate position of the transition state. ===&lt;br /&gt;
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Hammond&#039;s postulate essentially states that if 2 species are of similar energy they are of a similar structure. Thus in this reaction we can deduce that the transition state will be similar in structure to the reactants of the forward exothermic reaction, F and H2. By testing and varying the bond distances of F-H and H-H until the forces exterted on each other were 0 (characteristic in the transition state) the internuclear distances found were 1.811 Å for F-H and 0.745 for H-H Å.&lt;br /&gt;
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=== Question 3: Report the activation energy for both reactions. ===&lt;br /&gt;
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&lt;br /&gt;
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The activation energy can be easily calculated by taking away the reactant energy from the transition state energy. Using the internuclear distances of the atoms in the transition state calculated above in the settings function in the programme, the energy of the transition state was found to be -103.752 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;. The energy of the reactants, for the exothermic reaction for example, was found by inputting the normal bond length for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and making the distance between F and H relatively large so they&#039;re not interacting yielding the lowest energy for the reactants possible. From this the activation energies for the exothermic reaction was found to be 30.267 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; and the activation energy for the endothermic reaction was found to be 0.242 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;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 for the reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
&lt;br /&gt;
Due to the conservation of energy, all initial kinetic energy from the reactants&#039; momentum is converted and released as heat in the reaction once the products HF and H are formed. Due to the release of heat the surroundings temperature would increase as this is an exothermic reaction. This temperature change or increase in this case can be recorded by bomb calorimetry.&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 for the reaction HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For this endothermic reaction (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) there are two main modes of reactant energy to consider as the reactants approach the energy barrier/transition state point to form the products; these modes of energy are translational and vibrational energy. &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;Polanyi stated that for simple reactions described as an A + BC system, such as this H + HF system, if they have a late transition state, reactants with high vibrational energy is more effective for the reaction and its success, than reactants with high translational energy. This is because for a late transition state reaction, reactant molecules with high vibrational energy, if in the correct orientation, can vibrate their way to the top of the barrier, passing through the transition state forming the products successfully; however, if the reactants had high translational energy, in trying to reach the top of the energy barrier, they would just collide into the inner wall of the potential energy well and return to where they came from. This reaction being considered here (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) is an endothermic reaction with a late transition state as shown by the surface plot discussed earlier. Therefore to maximise the efficiency and the success of this reaction, reactants should have high vibrational energy. Polanyi also implied, that in this type of reaction (endothermic and late transition state), the products are likely to have high translational energy if the reaction effectively occurs with high vibrational energy reactants.&lt;br /&gt;
&lt;br /&gt;
The reaction showing highest efficiency and most effectiveness for its success was then modelled; high vibrational energy was inputted in the settings function for the molecule HF and high initial momentum of the incoming hydrogen atom for the collision was also inputted. However, unfortunately no such combination of momenta and bond length values were found that yielded a successful reaction, but below shows a contour plot with high vibrational energy in the reactants as shown by the oscillating trajectory which is what is needed to ensure high efficiency of this late transition state endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Loooool.png]]&lt;br /&gt;
&lt;br /&gt;
== References  ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; P. Atkins, J. De Paula, (n.d.). Physical chemistry. 7th edition.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics Prentice-Hall.&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794102</id>
		<title>MRD:Jsr3217</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:Jsr3217&amp;diff=794102"/>
		<updated>2019-06-03T14:23:51Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* 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;== H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System  ==&lt;br /&gt;
&lt;br /&gt;
If we define H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; as A and BC in our system, as the hydrogen atom collides with the hydrogen molecule, provided H has enough momentum and thus enough energy, the system changes and is described as AB and C where AB is our new diatomic product (A,B and C are the same type of atom).  &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;
&lt;br /&gt;
The transition state for this triatomic collision is a saddle point located at the intersection of the two potential energy surfaces, one PES for the Hydrogen atom and 1 PES for the Hydrogen molecule. The transition state is also a maximum on the trajectory pathway.&lt;br /&gt;
&lt;br /&gt;
Firstly the transition state being a turning point has a derivative of 0 with respect to q. This is shown by the following equation: (∂V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) and (∂V(q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)=0. However being a saddle point, the transition state is also defined as the point in the surface plot where there is a minimum in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction but also a maximum in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction, where q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are orthogonal to each other . This is where we have to take into account the second derivative of the potential energy V with respect to q. Mathematically these results are expressed as ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;gt;0 and ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)/∂q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; &amp;lt;0. The former second order differential equation refers to the minimum point in the q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; direction and the latter second order differential equation refers to the maximum point in the q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; direction.&lt;br /&gt;
&lt;br /&gt;
The transition state can be distinguished from a local minimum of the potential energy surface as by definition a local minimum will only have one 2nd derivative of potential energy (with respect to q in this case) which is greater than 0. However the transition state, being a saddle point, is a point with 2 second derivatives of potential energy in two different directions, one which is greater than 0 and one which is less than 0. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|I can tell from this explanation that you understand the shape of the TS on the PES however your discussion here is not quite complete as you haven&#039;t defined the directions q1 and q2 so you haven&#039;t fully defined the shape of the TS. A diagram with the vectors included would be really helpful here. In general diagrams are useful! [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 15:23, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Original Surface Plot showing both Potential Energy Surfaces and the Trajectory Pathway:&lt;br /&gt;
&lt;br /&gt;
[[File:1st surface plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the point where the interatomic distances are equal i.e. when the bond length of A-B is equal to the bond length of B-C. This is when the A-B bond is forming to make the diatomic product AB and the B-C bond is breaking leaving C on its own. This is shown below in the contour plot:&lt;br /&gt;
&lt;br /&gt;
[[File:1st contour plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== Question 2: What is 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;
&lt;br /&gt;
The position of the transition state can be found by varying the AB and BC distances, with both momentum values of AB and BC being 0, until no variation in the Internuclear Distances vs Time Plot is noticed or until a straight line in the plot is seen. No variation or oscillation in the plot means there are no vibrations which is what happens in the transition state. The distance at which no oscillation was seen was found to be at 0.90774 Å.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Internuclear Distance vs Time Plot at the transition state:&lt;br /&gt;
&lt;br /&gt;
[[File:2nd question graph 1.PNG]]&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;
&lt;br /&gt;
&lt;br /&gt;
The plot with the MEP calculation shows a relatively short line with little variation in the y-axis (AB distance) however, the plot with the Dynamics calculation shows an oscillating line. The trajectory for the dynamics calculated plot is also longer in length than the MEP calculated plot. This is due to the MEP calculation not considering any vibrational modes therefore no oscillations are shown on the plot. In actuality, atoms have mass and momentum and so the vibrations of the hydrogen molecule are taken into account shown by the oscillations in the dynamics calculation plot. Thus the model with the dynamics calculation is the more accurate one.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Plot with MEP Calculation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ACTUALMEP1.PNG]]&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Plot with Dynamics Calculation:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ACTUALDYNAMIC.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== Question 4: 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;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|+ Reactive or Unreactive Trajectories?&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the Trajectory !! Description &lt;br /&gt;
|-&lt;br /&gt;
| -1.25	|| -2.5	||-99.018 || Yes || [[File:1T.PNG]] ||Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products.|| &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.0	|| -100.456 || No || [[File:2T.PNG]] || Contour Plot shows that reaction does not occur as reactants don&#039;t have enough initial momentum and thus required (kinetic) energy to get over the activation energy barrier and reach the energy of the transition state. This is shown by the trajectory not reaching the transition state point and tailing back to the reactants. As the transition state isn&#039;t reached, the products aren&#039;t formed. || &lt;br /&gt;
|-&lt;br /&gt;
| -1.5	|| -2.5	|| -98.956|| Yes ||[[File:3T.PNG]] || Contour Plot shows a successful reaction with reactants, having passed through the transition state shown by the trajectory, fully converted into products. The reaction is successful as the reactants have enough initial momentum and thus energy to reach the energy of the transition state. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.0	|| -84.956 || No || [[File:4T.PNG]] || Contour Plot shows although he reactants have enough initial momentum and thus energy to go through the transition state, the transition state collapses back into the reactants. This happens because of barrier recrossing. ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5	|| -5.2	|| -83.416 || Yes || [[File:5T.PNG]] || Trajectory from contour plot shows that the reaction goes through/reaches the transition state point more than once. This occurs because of barrier recrossing again. However with these specific reaction conditions, the reaction does take place and the products are formed from the transition state. ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Question 5: State what are the main assumptions of Transition State Theory. 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;
&lt;br /&gt;
Transition State Theory assumes and tells us that states that &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; the transition state or activated complex in a reaction is in equilibrium with the reactants and once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. It also assumes the energy of the particles follows a Boltzmann distribution&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; but in this system since there are only 3 atoms in total for this triatomic collision there is no boltzmann distribution. As just mentioned, transition state theory assumes once the reactants turn into the activated complex, the complex doesn&#039;t return to the reactants. However in contour plot 4 above where the trajectory shows that although the reaction goes through the transition state, the reactants are still reformed. This is because of barrier recrossing as mentioned above; with this present, the rate of this reaction, experimentally determined, would be lower than the reaction rate that the transition state theory would predict.&lt;br /&gt;
&lt;br /&gt;
== F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
=== Question 1: 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;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:D1.PNG]]&lt;br /&gt;
&lt;br /&gt;
The above surface plot shows the potential energy surface for the exothermic conversion of F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to HF and H. The potential energy well slopes downwards from the reactants to the products showing that the energy of the products is lower than the energy of reactants. This reaction is an exothermic one as the bond strength of HF, the product, is stronger than the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactant. This means that the energy released from the formation of the HF bond is greater than the energy required to break the H-H bond in the hydrogen reactant molecule making the overall reaction exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:D2endo.PNG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The above surface plot shows the potential energy surface for the endothermic conversion of HF and H to H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F. This reaction is the reverse reaction of the exothermic conversion we&#039;ve just considered. This potenital energy well slopes upwards from the reactants to the products showing that the energy of the products is higher than the energy of reactants making the reaction endothermic. The energy released from the hydrogen molecule, the product, is less than the energy taken in to break in the H-F bond in the reactant making the overall reaction endothermic.&lt;br /&gt;
&lt;br /&gt;
=== Question 2: Locate the approximate position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate essentially states that if 2 species are of similar energy they are of a similar structure. Thus in this reaction we can deduce that the transition state will be similar in structure to the reactants of the forward exothermic reaction, F and H2. By testing and varying the bond distances of F-H and H-H until the forces exterted on each other were 0 (characteristic in the transition state) the internuclear distances found were 1.811 Å for F-H and 0.745 for H-H Å.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Question 3: Report the activation energy for both reactions. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The activation energy can be easily calculated by taking away the reactant energy from the transition state energy. Using the internuclear distances of the atoms in the transition state calculated above in the settings function in the programme, the energy of the transition state was found to be -103.752 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;. The energy of the reactants, for the exothermic reaction for example, was found by inputting the normal bond length for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and making the distance between F and H relatively large so they&#039;re not interacting yielding the lowest energy for the reactants possible. From this the activation energies for the exothermic reaction was found to be 30.267 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; and the activation energy for the endothermic reaction was found to be 0.242 kcal mol&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;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 for the reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; HF + H. Explain how this could be confirmed experimentally. ===&lt;br /&gt;
&lt;br /&gt;
Due to the conservation of energy, all initial kinetic energy from the reactants&#039; momentum is converted and released as heat in the reaction once the products HF and H are formed. Due to the release of heat the surroundings temperature would increase as this is an exothermic reaction. This temperature change or increase in this case can be recorded by bomb calorimetry.&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 for the reaction HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, and how this is influenced by the position of the transition state. ===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For this endothermic reaction (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) there are two main modes of reactant energy to consider as the reactants approach the energy barrier/transition state point to form the products; these modes of energy are translational and vibrational energy. &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;Polanyi stated that for simple reactions described as an A + BC system, such as this H + HF system, if they have a late transition state, reactants with high vibrational energy is more effective for the reaction and its success, than reactants with high translational energy. This is because for a late transition state reaction, reactant molecules with high vibrational energy, if in the correct orientation, can vibrate their way to the top of the barrier, passing through the transition state forming the products successfully; however, if the reactants had high translational energy, in trying to reach the top of the energy barrier, they would just collide into the inner wall of the potential energy well and return to where they came from. This reaction being considered here (HF + H -&amp;gt; F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) is an endothermic reaction with a late transition state as shown by the surface plot discussed earlier. Therefore to maximise the efficiency and the success of this reaction, reactants should have high vibrational energy. Polanyi also implied, that in this type of reaction (endothermic and late transition state), the products are likely to have high translational energy if the reaction effectively occurs with high vibrational energy reactants.&lt;br /&gt;
&lt;br /&gt;
The reaction showing highest efficiency and most effectiveness for its success was then modelled; high vibrational energy was inputted in the settings function for the molecule HF and high initial momentum of the incoming hydrogen atom for the collision was also inputted. However, unfortunately no such combination of momenta and bond length values were found that yielded a successful reaction, but below shows a contour plot with high vibrational energy in the reactants as shown by the oscillating trajectory which is what is needed to ensure high efficiency of this late transition state endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Loooool.png]]&lt;br /&gt;
&lt;br /&gt;
== References  ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; P. Atkins, J. De Paula, (n.d.). Physical chemistry. 7th edition.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; J. I. Steinfeld, J. S. Francisco, W. L. Hase Chemical Kinetic and Dynamics Prentice-Hall.&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794089</id>
		<title>Rrp17</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794089"/>
		<updated>2019-06-03T12:37:11Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Distribution of energy between different modes */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= &amp;lt;b&amp;gt;Molecular Reaction Dynamics &amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
= &amp;lt;b&amp;gt;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
If H collides with a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, there system can be defined as an AB and C.&lt;br /&gt;
{{fontcolor|pink| This is a slightly pointless statement as &amp;quot;an AB and C&amp;quot; doesn&#039;t really mean anything! Make sure you are always clear and spell everything out very explicitly, i.e. saying the atoms can be labelled... etc.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:25, 3 June 2019 (BST)}}&lt;br /&gt;
==== How is the transition state defined? ====&lt;br /&gt;
&lt;br /&gt;
The transition state is the maximum on the minimum energy path that links reactants to products; this point is where, ∂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, the gradient of the potential energy is zero and the distance r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; .  &lt;br /&gt;
&lt;br /&gt;
[[File:rrps_plot.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 1:&amp;lt;/b&amp;gt;The surface plot of the reaction between H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. The energies are represented by red and blue colours (high and low potential energy) and the black line is the trajectory of the reaction.|250px]]&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
It can be seen that the transition state can be distinguished from a local minimum by plotting a tangent at the inflection point of the minimum energy path. The first derivative, ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q1&amp;lt;sub&amp;gt;q1&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;gt;0and the second derivative ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q2&amp;lt;sub&amp;gt;q2&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;lt;0&lt;br /&gt;
This would give you a maximum however, a tangent perpendicular to the q&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; would derive the minimum; this location is known as the saddle point and thus the transition state of a reaction. The transition state is a saddle point, it is where the minimum , q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and max ,q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; intersect.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Yes, great understanding shown here. Also (I can infer you already know this from your answer but it&#039;s always good to be detailed so...) on the perpendicular tangent you mention on which the TS is a minimum, the second partial derivate would be positive as it is a minimum. Also make sure you say second partial derivative not just second derivative. Otherwise good. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:28, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is symmetric and hence, 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;, the momentum are zero and there is no gradient at the ridge. The location of the transition state can can be seen in plot 2 and the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) was found to be 0.9077 Å.&lt;br /&gt;
This was determined by choosing a random value of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and changing the inter-nuclear distance until the force equalled zero. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Good, but until what &amp;quot;force&amp;quot; equalled zero? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:29, 3 June 2019 (BST)}}&lt;br /&gt;
[[File:rrp17_i_t.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 2&amp;lt;/b&amp;gt; A plot of inter-nuclear distance vs time for the bond distance of 0.907 Å.|200px ]]&lt;br /&gt;
&lt;br /&gt;
====Minimum energy path and trajectory====&lt;br /&gt;
&lt;br /&gt;
The trajectory is a reaction path of minimum energy where the velocities/momenta are set to zero in each time step. This is where we displayed the transition state position by r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta is zero. This is shown in plot 3. &lt;br /&gt;
&lt;br /&gt;
However, MEP cannot characterise a reaction in terms of the motion of atoms. The reaction calculation under &#039;Dynamics&#039; that is shown in plot 4.&lt;br /&gt;
&lt;br /&gt;
It can be seen that the MEP plot is a plateaued line as the kinetic energy is reset to zero at every interval and, there molecules are not vibrating however, with the dynamic plot, the line is seen as oscillating as the molecules have momentum.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! MEP !! Dynamic !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:Rrpep.PNG|thumb|&amp;lt;b&amp;gt;Plot 3&amp;lt;/b&amp;gt; The MEP surface plot.|250px ]] || [[File:Rrpyn.PNG|thumb|&amp;lt;b&amp;gt;Plot 4&amp;lt;/b&amp;gt; The trajectory surface plot|250px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Good use of diagrams to explain and good understanding of the difference in the calculations. Make sure that at the very start of your explanation you are clear about what you are discussing. I.e. here instead of &amp;quot;The trajectory is a reaction path..&amp;quot; etc you should say &amp;quot;A MEP calculation computes the trajectory of minimum energy..&amp;quot; etc especially as you are comparing two methods it is good to be clear of which one we are talking about.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:31, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Reactive and nonreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ caption&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy (Kcal/mol) !! Reactive? !! Trajectory contour plot !! Dynamic description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || yes || [[File:rrpc1.PNG|thumb]] ||The trajectory passes through the transition state as the reaction has enough energy. The B-C bond breaks and the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2 || -100.456 || no ||[[File:RrpC2.PNG|thumb]] ||The trajectory does not pass through the activation barrier as there is not enough energy&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || yes || [[File:rrpc3.PNG|thumb]] ||The trajectory goes through the transition state as the reaction has sufficient energy to overcome the activation barrier and the B-C bond breaks whilst the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5 || -84.956 || no || [[File:rrpc4.PNG|thumb]] || The B-A bond formed however, the trajectory reverts back to the reactants and the B-C bond reforms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || yes || [[File:rrpc5.PNG|thumb]] || the B-A bond forms, only to revert back and re-form the B-C bond. Subsequently, the B-A bond forms again. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It is clear that the higher the total energy the more likely the reaction will go to completion as the energy is greater than the activation energy. However, it can be seen that with the last two contour plots, the products do not form-another variable affects the outcome of the reaction other than activation energy!&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Yep basically the determining factors about whether or not the system will be reactive is not as simple as a threshold energy value above which the reactants will react. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:33, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Assumptions of Transition State Theory====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory explains how the rate of a chemical reaction by which the reaction passes through a transition state and it has three assumptions:&lt;br /&gt;
&lt;br /&gt;
-The energy of the particles follow a Boltzmann distribution&lt;br /&gt;
-The reactants and transition state structure is in equilibrium&lt;br /&gt;
-The transition state structure does not revert back to the reactants once the reactants form the transition state&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Firstly, this should be cited. Secondly, while this is true, it doesn&#039;t fully answer the question - how would these assumptions affect the calculated rate of reaction and the comparison of this rate to real-life rates (the accuracy of it)?[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:33, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;Exercise 2: F-H-H system&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
Using the energy surface, the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction as the products are lower in energy than the reactants.This bond breaking process must mean that the H-F bond is stronger than the H-H and this relates t the ionic nature of the bond due to the large difference in electronegativity between the atoms. Thus, the reverse reaction must be endothermic.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpf.PNG|thumb|center|Surface plot of the F-H-H system with AB=HF and BC=H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====The approximate position of the transition state====&lt;br /&gt;
&lt;br /&gt;
Using a MEP contour plot, the saddle point (where there is no momentum) was determined. AB=1.908 Å , BC=0.745 Å. The use of an internuclear distance vs time also highlighted this.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Contour Plot !! Zoom of Contour !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpts.PNG|thumb|center|Contour plot of trajectory| 250px]]  || [[File:rrpzm.PNG|thumb| Trajectory zoomed in]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Activation energy====&lt;br /&gt;
&lt;br /&gt;
The activation energy for both reactions was determined by calculating the difference between the reactants/products and the transition state using an energy vs time plot .&lt;br /&gt;
&lt;br /&gt;
-For the H + HF reaction the activation energy was found to be 30 kcal/mol. &lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction the activation energy was found to be 0.026 kcal/mol. This was determined by zooming in on the energy vs time plot: number = 5000 and the BC distance was deviated to 1.82 angstroms and the activation energy is the difference between the total and potential energies.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:rrphf.PNG|thumb|center|Finding the activation energy for the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction|250px]]&lt;br /&gt;
[[File:rrphfa.PNG|thumb|center|Finding the activation energy for the H + HF reaction|250px]]&lt;br /&gt;
&lt;br /&gt;
====Mechanism for the release of the reaction energy====&lt;br /&gt;
&lt;br /&gt;
Given that this reaction is exothermic, the thermal energy released would result in an overall increase in kinetic energy and a fall of the potential. Moreover, this exothermic reaction can be determined with calorimetry with sufficient insulation to prevent heat loss.&lt;br /&gt;
&lt;br /&gt;
The initial conditions that result in a reactive trajectory:&lt;br /&gt;
HH distance of 0.74&lt;br /&gt;
HF distance of 2.3&lt;br /&gt;
HF momentum of -2.2&lt;br /&gt;
HH momentum of -1.9&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The results are shown below and show that the potential energy is a mirror of the kinetic energy and the potential energy converts to kinetic- this is how energy is conserved.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpcons.PNG|thumb|center|Energy vs Time |250px]]&lt;br /&gt;
[[File:rrpmvt.PNG|thumb|center|Momentum vs Time |250px]]&lt;br /&gt;
&lt;br /&gt;
====Distribution of energy between different modes====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rules&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; explain that the efficiency of the reaction is affected by the distribution of energy between different modes; an exothermic reaction has an early transition state and translational energy plays a more fundamental role than vibrational energy in the efficiency of the reaction and vice versa. The r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; momentum corresponds to the vibrational energy and the r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; corresponds to the translational energy.&lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction, it can be seen using a dynamic contour plot, when translational energy is greater than vibrational energy, the reaction is efficient and is complete. This exothermic reaction follows Polanyi&#039;s rules.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Incomplete !! Complete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrph2com.PNG|thumb| High translational energy leads to a complete reaction|250px]]  || [[File:rrph2non.PNG|thumb|Low translational energy does not lead to a complete reaction|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-For the HF + F reaction, the transition state is late and vibrational energy, according to Polyani&#039;s rules, is more important than translational and allows a more efficient reaction for this endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Complete !! inComplete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpyes.PNG|thumb|High vibrational energy, reaction complete|250px]]  || [[File:rrpno.PNG|thumb|Low vibrational energy, reaction incomplete|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
{{fontcolor|pink| Good understanding, explanation and use of examples.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:37, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;References&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
[1]Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction, Zhaojun Zhang, Yong Zhou,† and Dong H. Zhang, dx.doi.org/10.1021/jz301649w | J. Phys. Chem. Lett. 2012, 3, 3416−3419&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794088</id>
		<title>Rrp17</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794088"/>
		<updated>2019-06-03T12:33:58Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Assumptions of Transition State Theory */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= &amp;lt;b&amp;gt;Molecular Reaction Dynamics &amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
= &amp;lt;b&amp;gt;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
If H collides with a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, there system can be defined as an AB and C.&lt;br /&gt;
{{fontcolor|pink| This is a slightly pointless statement as &amp;quot;an AB and C&amp;quot; doesn&#039;t really mean anything! Make sure you are always clear and spell everything out very explicitly, i.e. saying the atoms can be labelled... etc.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:25, 3 June 2019 (BST)}}&lt;br /&gt;
==== How is the transition state defined? ====&lt;br /&gt;
&lt;br /&gt;
The transition state is the maximum on the minimum energy path that links reactants to products; this point is where, ∂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, the gradient of the potential energy is zero and the distance r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; .  &lt;br /&gt;
&lt;br /&gt;
[[File:rrps_plot.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 1:&amp;lt;/b&amp;gt;The surface plot of the reaction between H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. The energies are represented by red and blue colours (high and low potential energy) and the black line is the trajectory of the reaction.|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
It can be seen that the transition state can be distinguished from a local minimum by plotting a tangent at the inflection point of the minimum energy path. The first derivative, ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q1&amp;lt;sub&amp;gt;q1&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;gt;0and the second derivative ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q2&amp;lt;sub&amp;gt;q2&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;lt;0&lt;br /&gt;
This would give you a maximum however, a tangent perpendicular to the q&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; would derive the minimum; this location is known as the saddle point and thus the transition state of a reaction. The transition state is a saddle point, it is where the minimum , q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and max ,q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; intersect.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Yes, great understanding shown here. Also (I can infer you already know this from your answer but it&#039;s always good to be detailed so...) on the perpendicular tangent you mention on which the TS is a minimum, the second partial derivate would be positive as it is a minimum. Also make sure you say second partial derivative not just second derivative. Otherwise good. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:28, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is symmetric and hence, 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;, the momentum are zero and there is no gradient at the ridge. The location of the transition state can can be seen in plot 2 and the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) was found to be 0.9077 Å.&lt;br /&gt;
This was determined by choosing a random value of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and changing the inter-nuclear distance until the force equalled zero. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Good, but until what &amp;quot;force&amp;quot; equalled zero? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:29, 3 June 2019 (BST)}}&lt;br /&gt;
[[File:rrp17_i_t.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 2&amp;lt;/b&amp;gt; A plot of inter-nuclear distance vs time for the bond distance of 0.907 Å.|200px ]]&lt;br /&gt;
&lt;br /&gt;
====Minimum energy path and trajectory====&lt;br /&gt;
&lt;br /&gt;
The trajectory is a reaction path of minimum energy where the velocities/momenta are set to zero in each time step. This is where we displayed the transition state position by r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta is zero. This is shown in plot 3. &lt;br /&gt;
&lt;br /&gt;
However, MEP cannot characterise a reaction in terms of the motion of atoms. The reaction calculation under &#039;Dynamics&#039; that is shown in plot 4.&lt;br /&gt;
&lt;br /&gt;
It can be seen that the MEP plot is a plateaued line as the kinetic energy is reset to zero at every interval and, there molecules are not vibrating however, with the dynamic plot, the line is seen as oscillating as the molecules have momentum.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! MEP !! Dynamic !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:Rrpep.PNG|thumb|&amp;lt;b&amp;gt;Plot 3&amp;lt;/b&amp;gt; The MEP surface plot.|250px ]] || [[File:Rrpyn.PNG|thumb|&amp;lt;b&amp;gt;Plot 4&amp;lt;/b&amp;gt; The trajectory surface plot|250px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Good use of diagrams to explain and good understanding of the difference in the calculations. Make sure that at the very start of your explanation you are clear about what you are discussing. I.e. here instead of &amp;quot;The trajectory is a reaction path..&amp;quot; etc you should say &amp;quot;A MEP calculation computes the trajectory of minimum energy..&amp;quot; etc especially as you are comparing two methods it is good to be clear of which one we are talking about.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:31, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Reactive and nonreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ caption&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy (Kcal/mol) !! Reactive? !! Trajectory contour plot !! Dynamic description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || yes || [[File:rrpc1.PNG|thumb]] ||The trajectory passes through the transition state as the reaction has enough energy. The B-C bond breaks and the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2 || -100.456 || no ||[[File:RrpC2.PNG|thumb]] ||The trajectory does not pass through the activation barrier as there is not enough energy&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || yes || [[File:rrpc3.PNG|thumb]] ||The trajectory goes through the transition state as the reaction has sufficient energy to overcome the activation barrier and the B-C bond breaks whilst the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5 || -84.956 || no || [[File:rrpc4.PNG|thumb]] || The B-A bond formed however, the trajectory reverts back to the reactants and the B-C bond reforms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || yes || [[File:rrpc5.PNG|thumb]] || the B-A bond forms, only to revert back and re-form the B-C bond. Subsequently, the B-A bond forms again. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It is clear that the higher the total energy the more likely the reaction will go to completion as the energy is greater than the activation energy. However, it can be seen that with the last two contour plots, the products do not form-another variable affects the outcome of the reaction other than activation energy!&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Yep basically the determining factors about whether or not the system will be reactive is not as simple as a threshold energy value above which the reactants will react. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:33, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Assumptions of Transition State Theory====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory explains how the rate of a chemical reaction by which the reaction passes through a transition state and it has three assumptions:&lt;br /&gt;
&lt;br /&gt;
-The energy of the particles follow a Boltzmann distribution&lt;br /&gt;
-The reactants and transition state structure is in equilibrium&lt;br /&gt;
-The transition state structure does not revert back to the reactants once the reactants form the transition state&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Firstly, this should be cited. Secondly, while this is true, it doesn&#039;t fully answer the question - how would these assumptions affect the calculated rate of reaction and the comparison of this rate to real-life rates (the accuracy of it)?[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:33, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;Exercise 2: F-H-H system&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
Using the energy surface, the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction as the products are lower in energy than the reactants.This bond breaking process must mean that the H-F bond is stronger than the H-H and this relates t the ionic nature of the bond due to the large difference in electronegativity between the atoms. Thus, the reverse reaction must be endothermic.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpf.PNG|thumb|center|Surface plot of the F-H-H system with AB=HF and BC=H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====The approximate position of the transition state====&lt;br /&gt;
&lt;br /&gt;
Using a MEP contour plot, the saddle point (where there is no momentum) was determined. AB=1.908 Å , BC=0.745 Å. The use of an internuclear distance vs time also highlighted this.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Contour Plot !! Zoom of Contour !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpts.PNG|thumb|center|Contour plot of trajectory| 250px]]  || [[File:rrpzm.PNG|thumb| Trajectory zoomed in]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Activation energy====&lt;br /&gt;
&lt;br /&gt;
The activation energy for both reactions was determined by calculating the difference between the reactants/products and the transition state using an energy vs time plot .&lt;br /&gt;
&lt;br /&gt;
-For the H + HF reaction the activation energy was found to be 30 kcal/mol. &lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction the activation energy was found to be 0.026 kcal/mol. This was determined by zooming in on the energy vs time plot: number = 5000 and the BC distance was deviated to 1.82 angstroms and the activation energy is the difference between the total and potential energies.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:rrphf.PNG|thumb|center|Finding the activation energy for the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction|250px]]&lt;br /&gt;
[[File:rrphfa.PNG|thumb|center|Finding the activation energy for the H + HF reaction|250px]]&lt;br /&gt;
&lt;br /&gt;
====Mechanism for the release of the reaction energy====&lt;br /&gt;
&lt;br /&gt;
Given that this reaction is exothermic, the thermal energy released would result in an overall increase in kinetic energy and a fall of the potential. Moreover, this exothermic reaction can be determined with calorimetry with sufficient insulation to prevent heat loss.&lt;br /&gt;
&lt;br /&gt;
The initial conditions that result in a reactive trajectory:&lt;br /&gt;
HH distance of 0.74&lt;br /&gt;
HF distance of 2.3&lt;br /&gt;
HF momentum of -2.2&lt;br /&gt;
HH momentum of -1.9&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The results are shown below and show that the potential energy is a mirror of the kinetic energy and the potential energy converts to kinetic- this is how energy is conserved.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpcons.PNG|thumb|center|Energy vs Time |250px]]&lt;br /&gt;
[[File:rrpmvt.PNG|thumb|center|Momentum vs Time |250px]]&lt;br /&gt;
&lt;br /&gt;
====Distribution of energy between different modes====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rules&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; explain that the efficiency of the reaction is affected by the distribution of energy between different modes; an exothermic reaction has an early transition state and translational energy plays a more fundamental role than vibrational energy in the efficiency of the reaction and vice versa. The r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; momentum corresponds to the vibrational energy and the r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; corresponds to the translational energy.&lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction, it can be seen using a dynamic contour plot, when translational energy is greater than vibrational energy, the reaction is efficient and is complete. This exothermic reaction follows Polanyi&#039;s rules.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Incomplete !! Complete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrph2com.PNG|thumb| High translational energy leads to a complete reaction|250px]]  || [[File:rrph2non.PNG|thumb|Low translational energy does not lead to a complete reaction|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-For the HF + F reaction, the transition state is late and vibrational energy, according to Polyani&#039;s rules, is more important than translational and allows a more efficient reaction for this endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Complete !! inComplete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpyes.PNG|thumb|High vibrational energy, reaction complete|250px]]  || [[File:rrpno.PNG|thumb|Low vibrational energy, reaction incomplete|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;References&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
[1]Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction, Zhaojun Zhang, Yong Zhou,† and Dong H. Zhang, dx.doi.org/10.1021/jz301649w | J. Phys. Chem. Lett. 2012, 3, 3416−3419&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794087</id>
		<title>Rrp17</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794087"/>
		<updated>2019-06-03T12:33:01Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Reactive and nonreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= &amp;lt;b&amp;gt;Molecular Reaction Dynamics &amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
= &amp;lt;b&amp;gt;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
If H collides with a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, there system can be defined as an AB and C.&lt;br /&gt;
{{fontcolor|pink| This is a slightly pointless statement as &amp;quot;an AB and C&amp;quot; doesn&#039;t really mean anything! Make sure you are always clear and spell everything out very explicitly, i.e. saying the atoms can be labelled... etc.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:25, 3 June 2019 (BST)}}&lt;br /&gt;
==== How is the transition state defined? ====&lt;br /&gt;
&lt;br /&gt;
The transition state is the maximum on the minimum energy path that links reactants to products; this point is where, ∂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, the gradient of the potential energy is zero and the distance r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; .  &lt;br /&gt;
&lt;br /&gt;
[[File:rrps_plot.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 1:&amp;lt;/b&amp;gt;The surface plot of the reaction between H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. The energies are represented by red and blue colours (high and low potential energy) and the black line is the trajectory of the reaction.|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
It can be seen that the transition state can be distinguished from a local minimum by plotting a tangent at the inflection point of the minimum energy path. The first derivative, ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q1&amp;lt;sub&amp;gt;q1&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;gt;0and the second derivative ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q2&amp;lt;sub&amp;gt;q2&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;lt;0&lt;br /&gt;
This would give you a maximum however, a tangent perpendicular to the q&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; would derive the minimum; this location is known as the saddle point and thus the transition state of a reaction. The transition state is a saddle point, it is where the minimum , q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and max ,q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; intersect.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Yes, great understanding shown here. Also (I can infer you already know this from your answer but it&#039;s always good to be detailed so...) on the perpendicular tangent you mention on which the TS is a minimum, the second partial derivate would be positive as it is a minimum. Also make sure you say second partial derivative not just second derivative. Otherwise good. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:28, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is symmetric and hence, 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;, the momentum are zero and there is no gradient at the ridge. The location of the transition state can can be seen in plot 2 and the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) was found to be 0.9077 Å.&lt;br /&gt;
This was determined by choosing a random value of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and changing the inter-nuclear distance until the force equalled zero. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Good, but until what &amp;quot;force&amp;quot; equalled zero? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:29, 3 June 2019 (BST)}}&lt;br /&gt;
[[File:rrp17_i_t.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 2&amp;lt;/b&amp;gt; A plot of inter-nuclear distance vs time for the bond distance of 0.907 Å.|200px ]]&lt;br /&gt;
&lt;br /&gt;
====Minimum energy path and trajectory====&lt;br /&gt;
&lt;br /&gt;
The trajectory is a reaction path of minimum energy where the velocities/momenta are set to zero in each time step. This is where we displayed the transition state position by r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta is zero. This is shown in plot 3. &lt;br /&gt;
&lt;br /&gt;
However, MEP cannot characterise a reaction in terms of the motion of atoms. The reaction calculation under &#039;Dynamics&#039; that is shown in plot 4.&lt;br /&gt;
&lt;br /&gt;
It can be seen that the MEP plot is a plateaued line as the kinetic energy is reset to zero at every interval and, there molecules are not vibrating however, with the dynamic plot, the line is seen as oscillating as the molecules have momentum.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! MEP !! Dynamic !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:Rrpep.PNG|thumb|&amp;lt;b&amp;gt;Plot 3&amp;lt;/b&amp;gt; The MEP surface plot.|250px ]] || [[File:Rrpyn.PNG|thumb|&amp;lt;b&amp;gt;Plot 4&amp;lt;/b&amp;gt; The trajectory surface plot|250px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Good use of diagrams to explain and good understanding of the difference in the calculations. Make sure that at the very start of your explanation you are clear about what you are discussing. I.e. here instead of &amp;quot;The trajectory is a reaction path..&amp;quot; etc you should say &amp;quot;A MEP calculation computes the trajectory of minimum energy..&amp;quot; etc especially as you are comparing two methods it is good to be clear of which one we are talking about.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:31, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Reactive and nonreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ caption&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy (Kcal/mol) !! Reactive? !! Trajectory contour plot !! Dynamic description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || yes || [[File:rrpc1.PNG|thumb]] ||The trajectory passes through the transition state as the reaction has enough energy. The B-C bond breaks and the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2 || -100.456 || no ||[[File:RrpC2.PNG|thumb]] ||The trajectory does not pass through the activation barrier as there is not enough energy&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || yes || [[File:rrpc3.PNG|thumb]] ||The trajectory goes through the transition state as the reaction has sufficient energy to overcome the activation barrier and the B-C bond breaks whilst the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5 || -84.956 || no || [[File:rrpc4.PNG|thumb]] || The B-A bond formed however, the trajectory reverts back to the reactants and the B-C bond reforms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || yes || [[File:rrpc5.PNG|thumb]] || the B-A bond forms, only to revert back and re-form the B-C bond. Subsequently, the B-A bond forms again. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It is clear that the higher the total energy the more likely the reaction will go to completion as the energy is greater than the activation energy. However, it can be seen that with the last two contour plots, the products do not form-another variable affects the outcome of the reaction other than activation energy!&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Yep basically the determining factors about whether or not the system will be reactive is not as simple as a threshold energy value above which the reactants will react. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:33, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Assumptions of Transition State Theory====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory explains how the rate of a chemical reaction by which the reaction passes through a transition state and it has three assumptions:&lt;br /&gt;
&lt;br /&gt;
-The energy of the particles follow a Boltzmann distribution&lt;br /&gt;
-The reactants and transition state structure is in equilibrium&lt;br /&gt;
-The transition state structure does not revert back to the reactants once the reactants form the transition state&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;Exercise 2: F-H-H system&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
Using the energy surface, the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction as the products are lower in energy than the reactants.This bond breaking process must mean that the H-F bond is stronger than the H-H and this relates t the ionic nature of the bond due to the large difference in electronegativity between the atoms. Thus, the reverse reaction must be endothermic.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpf.PNG|thumb|center|Surface plot of the F-H-H system with AB=HF and BC=H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====The approximate position of the transition state====&lt;br /&gt;
&lt;br /&gt;
Using a MEP contour plot, the saddle point (where there is no momentum) was determined. AB=1.908 Å , BC=0.745 Å. The use of an internuclear distance vs time also highlighted this.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Contour Plot !! Zoom of Contour !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpts.PNG|thumb|center|Contour plot of trajectory| 250px]]  || [[File:rrpzm.PNG|thumb| Trajectory zoomed in]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Activation energy====&lt;br /&gt;
&lt;br /&gt;
The activation energy for both reactions was determined by calculating the difference between the reactants/products and the transition state using an energy vs time plot .&lt;br /&gt;
&lt;br /&gt;
-For the H + HF reaction the activation energy was found to be 30 kcal/mol. &lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction the activation energy was found to be 0.026 kcal/mol. This was determined by zooming in on the energy vs time plot: number = 5000 and the BC distance was deviated to 1.82 angstroms and the activation energy is the difference between the total and potential energies.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:rrphf.PNG|thumb|center|Finding the activation energy for the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction|250px]]&lt;br /&gt;
[[File:rrphfa.PNG|thumb|center|Finding the activation energy for the H + HF reaction|250px]]&lt;br /&gt;
&lt;br /&gt;
====Mechanism for the release of the reaction energy====&lt;br /&gt;
&lt;br /&gt;
Given that this reaction is exothermic, the thermal energy released would result in an overall increase in kinetic energy and a fall of the potential. Moreover, this exothermic reaction can be determined with calorimetry with sufficient insulation to prevent heat loss.&lt;br /&gt;
&lt;br /&gt;
The initial conditions that result in a reactive trajectory:&lt;br /&gt;
HH distance of 0.74&lt;br /&gt;
HF distance of 2.3&lt;br /&gt;
HF momentum of -2.2&lt;br /&gt;
HH momentum of -1.9&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The results are shown below and show that the potential energy is a mirror of the kinetic energy and the potential energy converts to kinetic- this is how energy is conserved.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpcons.PNG|thumb|center|Energy vs Time |250px]]&lt;br /&gt;
[[File:rrpmvt.PNG|thumb|center|Momentum vs Time |250px]]&lt;br /&gt;
&lt;br /&gt;
====Distribution of energy between different modes====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rules&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; explain that the efficiency of the reaction is affected by the distribution of energy between different modes; an exothermic reaction has an early transition state and translational energy plays a more fundamental role than vibrational energy in the efficiency of the reaction and vice versa. The r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; momentum corresponds to the vibrational energy and the r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; corresponds to the translational energy.&lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction, it can be seen using a dynamic contour plot, when translational energy is greater than vibrational energy, the reaction is efficient and is complete. This exothermic reaction follows Polanyi&#039;s rules.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Incomplete !! Complete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrph2com.PNG|thumb| High translational energy leads to a complete reaction|250px]]  || [[File:rrph2non.PNG|thumb|Low translational energy does not lead to a complete reaction|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-For the HF + F reaction, the transition state is late and vibrational energy, according to Polyani&#039;s rules, is more important than translational and allows a more efficient reaction for this endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Complete !! inComplete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpyes.PNG|thumb|High vibrational energy, reaction complete|250px]]  || [[File:rrpno.PNG|thumb|Low vibrational energy, reaction incomplete|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;References&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
[1]Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction, Zhaojun Zhang, Yong Zhou,† and Dong H. Zhang, dx.doi.org/10.1021/jz301649w | J. Phys. Chem. Lett. 2012, 3, 3416−3419&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794086</id>
		<title>Rrp17</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794086"/>
		<updated>2019-06-03T12:31:35Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Minimum energy path and trajectory */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= &amp;lt;b&amp;gt;Molecular Reaction Dynamics &amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
= &amp;lt;b&amp;gt;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
If H collides with a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, there system can be defined as an AB and C.&lt;br /&gt;
{{fontcolor|pink| This is a slightly pointless statement as &amp;quot;an AB and C&amp;quot; doesn&#039;t really mean anything! Make sure you are always clear and spell everything out very explicitly, i.e. saying the atoms can be labelled... etc.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:25, 3 June 2019 (BST)}}&lt;br /&gt;
==== How is the transition state defined? ====&lt;br /&gt;
&lt;br /&gt;
The transition state is the maximum on the minimum energy path that links reactants to products; this point is where, ∂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, the gradient of the potential energy is zero and the distance r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; .  &lt;br /&gt;
&lt;br /&gt;
[[File:rrps_plot.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 1:&amp;lt;/b&amp;gt;The surface plot of the reaction between H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. The energies are represented by red and blue colours (high and low potential energy) and the black line is the trajectory of the reaction.|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
It can be seen that the transition state can be distinguished from a local minimum by plotting a tangent at the inflection point of the minimum energy path. The first derivative, ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q1&amp;lt;sub&amp;gt;q1&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;gt;0and the second derivative ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q2&amp;lt;sub&amp;gt;q2&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;lt;0&lt;br /&gt;
This would give you a maximum however, a tangent perpendicular to the q&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; would derive the minimum; this location is known as the saddle point and thus the transition state of a reaction. The transition state is a saddle point, it is where the minimum , q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and max ,q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; intersect.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Yes, great understanding shown here. Also (I can infer you already know this from your answer but it&#039;s always good to be detailed so...) on the perpendicular tangent you mention on which the TS is a minimum, the second partial derivate would be positive as it is a minimum. Also make sure you say second partial derivative not just second derivative. Otherwise good. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:28, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is symmetric and hence, 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;, the momentum are zero and there is no gradient at the ridge. The location of the transition state can can be seen in plot 2 and the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) was found to be 0.9077 Å.&lt;br /&gt;
This was determined by choosing a random value of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and changing the inter-nuclear distance until the force equalled zero. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Good, but until what &amp;quot;force&amp;quot; equalled zero? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:29, 3 June 2019 (BST)}}&lt;br /&gt;
[[File:rrp17_i_t.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 2&amp;lt;/b&amp;gt; A plot of inter-nuclear distance vs time for the bond distance of 0.907 Å.|200px ]]&lt;br /&gt;
&lt;br /&gt;
====Minimum energy path and trajectory====&lt;br /&gt;
&lt;br /&gt;
The trajectory is a reaction path of minimum energy where the velocities/momenta are set to zero in each time step. This is where we displayed the transition state position by r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta is zero. This is shown in plot 3. &lt;br /&gt;
&lt;br /&gt;
However, MEP cannot characterise a reaction in terms of the motion of atoms. The reaction calculation under &#039;Dynamics&#039; that is shown in plot 4.&lt;br /&gt;
&lt;br /&gt;
It can be seen that the MEP plot is a plateaued line as the kinetic energy is reset to zero at every interval and, there molecules are not vibrating however, with the dynamic plot, the line is seen as oscillating as the molecules have momentum.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! MEP !! Dynamic !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:Rrpep.PNG|thumb|&amp;lt;b&amp;gt;Plot 3&amp;lt;/b&amp;gt; The MEP surface plot.|250px ]] || [[File:Rrpyn.PNG|thumb|&amp;lt;b&amp;gt;Plot 4&amp;lt;/b&amp;gt; The trajectory surface plot|250px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Good use of diagrams to explain and good understanding of the difference in the calculations. Make sure that at the very start of your explanation you are clear about what you are discussing. I.e. here instead of &amp;quot;The trajectory is a reaction path..&amp;quot; etc you should say &amp;quot;A MEP calculation computes the trajectory of minimum energy..&amp;quot; etc especially as you are comparing two methods it is good to be clear of which one we are talking about.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:31, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====Reactive and nonreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ caption&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy (Kcal/mol) !! Reactive? !! Trajectory contour plot !! Dynamic description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || yes || [[File:rrpc1.PNG|thumb]] ||The trajectory passes through the transition state as the reaction has enough energy. The B-C bond breaks and the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2 || -100.456 || no ||[[File:RrpC2.PNG|thumb]] ||The trajectory does not pass through the activation barrier as there is not enough energy&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || yes || [[File:rrpc3.PNG|thumb]] ||The trajectory goes through the transition state as the reaction has sufficient energy to overcome the activation barrier and the B-C bond breaks whilst the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5 || -84.956 || no || [[File:rrpc4.PNG|thumb]] || The B-A bond formed however, the trajectory reverts back to the reactants and the B-C bond reforms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || yes || [[File:rrpc5.PNG|thumb]] || the B-A bond forms, only to revert back and re-form the B-C bond. Subsequently, the B-A bond forms again. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It is clear that the higher the total energy the more likely the reaction will go to completion as the energy is greater than the activation energy. However, it can be seen that with the last two contour plots, the products do not form-another variable affects the outcome of the reaction other than activation energy!&lt;br /&gt;
&lt;br /&gt;
====Assumptions of Transition State Theory====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory explains how the rate of a chemical reaction by which the reaction passes through a transition state and it has three assumptions:&lt;br /&gt;
&lt;br /&gt;
-The energy of the particles follow a Boltzmann distribution&lt;br /&gt;
-The reactants and transition state structure is in equilibrium&lt;br /&gt;
-The transition state structure does not revert back to the reactants once the reactants form the transition state&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;Exercise 2: F-H-H system&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
Using the energy surface, the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction as the products are lower in energy than the reactants.This bond breaking process must mean that the H-F bond is stronger than the H-H and this relates t the ionic nature of the bond due to the large difference in electronegativity between the atoms. Thus, the reverse reaction must be endothermic.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpf.PNG|thumb|center|Surface plot of the F-H-H system with AB=HF and BC=H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====The approximate position of the transition state====&lt;br /&gt;
&lt;br /&gt;
Using a MEP contour plot, the saddle point (where there is no momentum) was determined. AB=1.908 Å , BC=0.745 Å. The use of an internuclear distance vs time also highlighted this.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Contour Plot !! Zoom of Contour !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpts.PNG|thumb|center|Contour plot of trajectory| 250px]]  || [[File:rrpzm.PNG|thumb| Trajectory zoomed in]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Activation energy====&lt;br /&gt;
&lt;br /&gt;
The activation energy for both reactions was determined by calculating the difference between the reactants/products and the transition state using an energy vs time plot .&lt;br /&gt;
&lt;br /&gt;
-For the H + HF reaction the activation energy was found to be 30 kcal/mol. &lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction the activation energy was found to be 0.026 kcal/mol. This was determined by zooming in on the energy vs time plot: number = 5000 and the BC distance was deviated to 1.82 angstroms and the activation energy is the difference between the total and potential energies.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:rrphf.PNG|thumb|center|Finding the activation energy for the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction|250px]]&lt;br /&gt;
[[File:rrphfa.PNG|thumb|center|Finding the activation energy for the H + HF reaction|250px]]&lt;br /&gt;
&lt;br /&gt;
====Mechanism for the release of the reaction energy====&lt;br /&gt;
&lt;br /&gt;
Given that this reaction is exothermic, the thermal energy released would result in an overall increase in kinetic energy and a fall of the potential. Moreover, this exothermic reaction can be determined with calorimetry with sufficient insulation to prevent heat loss.&lt;br /&gt;
&lt;br /&gt;
The initial conditions that result in a reactive trajectory:&lt;br /&gt;
HH distance of 0.74&lt;br /&gt;
HF distance of 2.3&lt;br /&gt;
HF momentum of -2.2&lt;br /&gt;
HH momentum of -1.9&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The results are shown below and show that the potential energy is a mirror of the kinetic energy and the potential energy converts to kinetic- this is how energy is conserved.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpcons.PNG|thumb|center|Energy vs Time |250px]]&lt;br /&gt;
[[File:rrpmvt.PNG|thumb|center|Momentum vs Time |250px]]&lt;br /&gt;
&lt;br /&gt;
====Distribution of energy between different modes====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rules&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; explain that the efficiency of the reaction is affected by the distribution of energy between different modes; an exothermic reaction has an early transition state and translational energy plays a more fundamental role than vibrational energy in the efficiency of the reaction and vice versa. The r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; momentum corresponds to the vibrational energy and the r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; corresponds to the translational energy.&lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction, it can be seen using a dynamic contour plot, when translational energy is greater than vibrational energy, the reaction is efficient and is complete. This exothermic reaction follows Polanyi&#039;s rules.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Incomplete !! Complete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrph2com.PNG|thumb| High translational energy leads to a complete reaction|250px]]  || [[File:rrph2non.PNG|thumb|Low translational energy does not lead to a complete reaction|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-For the HF + F reaction, the transition state is late and vibrational energy, according to Polyani&#039;s rules, is more important than translational and allows a more efficient reaction for this endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Complete !! inComplete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpyes.PNG|thumb|High vibrational energy, reaction complete|250px]]  || [[File:rrpno.PNG|thumb|Low vibrational energy, reaction incomplete|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;References&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
[1]Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction, Zhaojun Zhang, Yong Zhou,† and Dong H. Zhang, dx.doi.org/10.1021/jz301649w | J. Phys. Chem. Lett. 2012, 3, 3416−3419&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794085</id>
		<title>Rrp17</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794085"/>
		<updated>2019-06-03T12:29:16Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* EXERCISE 1: H + H2 system */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= &amp;lt;b&amp;gt;Molecular Reaction Dynamics &amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
= &amp;lt;b&amp;gt;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
If H collides with a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, there system can be defined as an AB and C.&lt;br /&gt;
{{fontcolor|pink| This is a slightly pointless statement as &amp;quot;an AB and C&amp;quot; doesn&#039;t really mean anything! Make sure you are always clear and spell everything out very explicitly, i.e. saying the atoms can be labelled... etc.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:25, 3 June 2019 (BST)}}&lt;br /&gt;
==== How is the transition state defined? ====&lt;br /&gt;
&lt;br /&gt;
The transition state is the maximum on the minimum energy path that links reactants to products; this point is where, ∂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, the gradient of the potential energy is zero and the distance r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; .  &lt;br /&gt;
&lt;br /&gt;
[[File:rrps_plot.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 1:&amp;lt;/b&amp;gt;The surface plot of the reaction between H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. The energies are represented by red and blue colours (high and low potential energy) and the black line is the trajectory of the reaction.|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
It can be seen that the transition state can be distinguished from a local minimum by plotting a tangent at the inflection point of the minimum energy path. The first derivative, ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q1&amp;lt;sub&amp;gt;q1&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;gt;0and the second derivative ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q2&amp;lt;sub&amp;gt;q2&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;lt;0&lt;br /&gt;
This would give you a maximum however, a tangent perpendicular to the q&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; would derive the minimum; this location is known as the saddle point and thus the transition state of a reaction. The transition state is a saddle point, it is where the minimum , q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and max ,q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; intersect.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Yes, great understanding shown here. Also (I can infer you already know this from your answer but it&#039;s always good to be detailed so...) on the perpendicular tangent you mention on which the TS is a minimum, the second partial derivate would be positive as it is a minimum. Also make sure you say second partial derivative not just second derivative. Otherwise good. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:28, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is symmetric and hence, 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;, the momentum are zero and there is no gradient at the ridge. The location of the transition state can can be seen in plot 2 and the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) was found to be 0.9077 Å.&lt;br /&gt;
This was determined by choosing a random value of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and changing the inter-nuclear distance until the force equalled zero. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Good, but until what &amp;quot;force&amp;quot; equalled zero? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:29, 3 June 2019 (BST)}}&lt;br /&gt;
[[File:rrp17_i_t.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 2&amp;lt;/b&amp;gt; A plot of inter-nuclear distance vs time for the bond distance of 0.907 Å.|200px ]]&lt;br /&gt;
&lt;br /&gt;
====Minimum energy path and trajectory====&lt;br /&gt;
&lt;br /&gt;
The trajectory is a reaction path of minimum energy where the velocities/momenta are set to zero in each time step. This is where we displayed the transition state position by r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta is zero. This is shown in plot 3. &lt;br /&gt;
&lt;br /&gt;
However, MEP cannot characterise a reaction in terms of the motion of atoms. The reaction calculation under &#039;Dynamics&#039; that is shown in plot 4.&lt;br /&gt;
&lt;br /&gt;
It can be seen that the MEP plot is a plateaued line as the kinetic energy is reset to zero at every interval and, there molecules are not vibrating however, with the dynamic plot, the line is seen as oscillating as the molecules have momentum.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! MEP !! Dynamic !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:Rrpep.PNG|thumb|&amp;lt;b&amp;gt;Plot 3&amp;lt;/b&amp;gt; The MEP surface plot.|250px ]] || [[File:Rrpyn.PNG|thumb|&amp;lt;b&amp;gt;Plot 4&amp;lt;/b&amp;gt; The trajectory surface plot|250px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Reactive and nonreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ caption&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy (Kcal/mol) !! Reactive? !! Trajectory contour plot !! Dynamic description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || yes || [[File:rrpc1.PNG|thumb]] ||The trajectory passes through the transition state as the reaction has enough energy. The B-C bond breaks and the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2 || -100.456 || no ||[[File:RrpC2.PNG|thumb]] ||The trajectory does not pass through the activation barrier as there is not enough energy&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || yes || [[File:rrpc3.PNG|thumb]] ||The trajectory goes through the transition state as the reaction has sufficient energy to overcome the activation barrier and the B-C bond breaks whilst the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5 || -84.956 || no || [[File:rrpc4.PNG|thumb]] || The B-A bond formed however, the trajectory reverts back to the reactants and the B-C bond reforms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || yes || [[File:rrpc5.PNG|thumb]] || the B-A bond forms, only to revert back and re-form the B-C bond. Subsequently, the B-A bond forms again. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It is clear that the higher the total energy the more likely the reaction will go to completion as the energy is greater than the activation energy. However, it can be seen that with the last two contour plots, the products do not form-another variable affects the outcome of the reaction other than activation energy!&lt;br /&gt;
&lt;br /&gt;
====Assumptions of Transition State Theory====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory explains how the rate of a chemical reaction by which the reaction passes through a transition state and it has three assumptions:&lt;br /&gt;
&lt;br /&gt;
-The energy of the particles follow a Boltzmann distribution&lt;br /&gt;
-The reactants and transition state structure is in equilibrium&lt;br /&gt;
-The transition state structure does not revert back to the reactants once the reactants form the transition state&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;Exercise 2: F-H-H system&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
Using the energy surface, the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction as the products are lower in energy than the reactants.This bond breaking process must mean that the H-F bond is stronger than the H-H and this relates t the ionic nature of the bond due to the large difference in electronegativity between the atoms. Thus, the reverse reaction must be endothermic.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpf.PNG|thumb|center|Surface plot of the F-H-H system with AB=HF and BC=H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====The approximate position of the transition state====&lt;br /&gt;
&lt;br /&gt;
Using a MEP contour plot, the saddle point (where there is no momentum) was determined. AB=1.908 Å , BC=0.745 Å. The use of an internuclear distance vs time also highlighted this.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Contour Plot !! Zoom of Contour !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpts.PNG|thumb|center|Contour plot of trajectory| 250px]]  || [[File:rrpzm.PNG|thumb| Trajectory zoomed in]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Activation energy====&lt;br /&gt;
&lt;br /&gt;
The activation energy for both reactions was determined by calculating the difference between the reactants/products and the transition state using an energy vs time plot .&lt;br /&gt;
&lt;br /&gt;
-For the H + HF reaction the activation energy was found to be 30 kcal/mol. &lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction the activation energy was found to be 0.026 kcal/mol. This was determined by zooming in on the energy vs time plot: number = 5000 and the BC distance was deviated to 1.82 angstroms and the activation energy is the difference between the total and potential energies.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:rrphf.PNG|thumb|center|Finding the activation energy for the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction|250px]]&lt;br /&gt;
[[File:rrphfa.PNG|thumb|center|Finding the activation energy for the H + HF reaction|250px]]&lt;br /&gt;
&lt;br /&gt;
====Mechanism for the release of the reaction energy====&lt;br /&gt;
&lt;br /&gt;
Given that this reaction is exothermic, the thermal energy released would result in an overall increase in kinetic energy and a fall of the potential. Moreover, this exothermic reaction can be determined with calorimetry with sufficient insulation to prevent heat loss.&lt;br /&gt;
&lt;br /&gt;
The initial conditions that result in a reactive trajectory:&lt;br /&gt;
HH distance of 0.74&lt;br /&gt;
HF distance of 2.3&lt;br /&gt;
HF momentum of -2.2&lt;br /&gt;
HH momentum of -1.9&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The results are shown below and show that the potential energy is a mirror of the kinetic energy and the potential energy converts to kinetic- this is how energy is conserved.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpcons.PNG|thumb|center|Energy vs Time |250px]]&lt;br /&gt;
[[File:rrpmvt.PNG|thumb|center|Momentum vs Time |250px]]&lt;br /&gt;
&lt;br /&gt;
====Distribution of energy between different modes====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rules&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; explain that the efficiency of the reaction is affected by the distribution of energy between different modes; an exothermic reaction has an early transition state and translational energy plays a more fundamental role than vibrational energy in the efficiency of the reaction and vice versa. The r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; momentum corresponds to the vibrational energy and the r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; corresponds to the translational energy.&lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction, it can be seen using a dynamic contour plot, when translational energy is greater than vibrational energy, the reaction is efficient and is complete. This exothermic reaction follows Polanyi&#039;s rules.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Incomplete !! Complete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrph2com.PNG|thumb| High translational energy leads to a complete reaction|250px]]  || [[File:rrph2non.PNG|thumb|Low translational energy does not lead to a complete reaction|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-For the HF + F reaction, the transition state is late and vibrational energy, according to Polyani&#039;s rules, is more important than translational and allows a more efficient reaction for this endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Complete !! inComplete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpyes.PNG|thumb|High vibrational energy, reaction complete|250px]]  || [[File:rrpno.PNG|thumb|Low vibrational energy, reaction incomplete|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;References&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
[1]Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction, Zhaojun Zhang, Yong Zhou,† and Dong H. Zhang, dx.doi.org/10.1021/jz301649w | J. Phys. Chem. Lett. 2012, 3, 3416−3419&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794084</id>
		<title>Rrp17</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794084"/>
		<updated>2019-06-03T12:29:07Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Transition state position */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= &amp;lt;b&amp;gt;Molecular Reaction Dynamics &amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
= &amp;lt;b&amp;gt;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
If H collides with a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, there system can be defined as an AB and C.&lt;br /&gt;
{{{{fontcolor|pink| This is a slightly pointless statement as &amp;quot;an AB and C&amp;quot; doesn&#039;t really mean anything! Make sure you are always clear and spell everything out very explicitly, i.e. saying the atoms can be labelled... etc.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:25, 3 June 2019 (BST)}}&lt;br /&gt;
==== How is the transition state defined? ====&lt;br /&gt;
&lt;br /&gt;
The transition state is the maximum on the minimum energy path that links reactants to products; this point is where, ∂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, the gradient of the potential energy is zero and the distance r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; .  &lt;br /&gt;
&lt;br /&gt;
[[File:rrps_plot.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 1:&amp;lt;/b&amp;gt;The surface plot of the reaction between H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. The energies are represented by red and blue colours (high and low potential energy) and the black line is the trajectory of the reaction.|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
It can be seen that the transition state can be distinguished from a local minimum by plotting a tangent at the inflection point of the minimum energy path. The first derivative, ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q1&amp;lt;sub&amp;gt;q1&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;gt;0and the second derivative ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q2&amp;lt;sub&amp;gt;q2&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;lt;0&lt;br /&gt;
This would give you a maximum however, a tangent perpendicular to the q&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; would derive the minimum; this location is known as the saddle point and thus the transition state of a reaction. The transition state is a saddle point, it is where the minimum , q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and max ,q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; intersect.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Yes, great understanding shown here. Also (I can infer you already know this from your answer but it&#039;s always good to be detailed so...) on the perpendicular tangent you mention on which the TS is a minimum, the second partial derivate would be positive as it is a minimum. Also make sure you say second partial derivative not just second derivative. Otherwise good. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:28, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is symmetric and hence, 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;, the momentum are zero and there is no gradient at the ridge. The location of the transition state can can be seen in plot 2 and the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) was found to be 0.9077 Å.&lt;br /&gt;
This was determined by choosing a random value of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and changing the inter-nuclear distance until the force equalled zero. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Good, but until what &amp;quot;force&amp;quot; equalled zero? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:29, 3 June 2019 (BST)}}&lt;br /&gt;
[[File:rrp17_i_t.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 2&amp;lt;/b&amp;gt; A plot of inter-nuclear distance vs time for the bond distance of 0.907 Å.|200px ]]&lt;br /&gt;
&lt;br /&gt;
====Minimum energy path and trajectory====&lt;br /&gt;
&lt;br /&gt;
The trajectory is a reaction path of minimum energy where the velocities/momenta are set to zero in each time step. This is where we displayed the transition state position by r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta is zero. This is shown in plot 3. &lt;br /&gt;
&lt;br /&gt;
However, MEP cannot characterise a reaction in terms of the motion of atoms. The reaction calculation under &#039;Dynamics&#039; that is shown in plot 4.&lt;br /&gt;
&lt;br /&gt;
It can be seen that the MEP plot is a plateaued line as the kinetic energy is reset to zero at every interval and, there molecules are not vibrating however, with the dynamic plot, the line is seen as oscillating as the molecules have momentum.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! MEP !! Dynamic !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:Rrpep.PNG|thumb|&amp;lt;b&amp;gt;Plot 3&amp;lt;/b&amp;gt; The MEP surface plot.|250px ]] || [[File:Rrpyn.PNG|thumb|&amp;lt;b&amp;gt;Plot 4&amp;lt;/b&amp;gt; The trajectory surface plot|250px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Reactive and nonreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ caption&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy (Kcal/mol) !! Reactive? !! Trajectory contour plot !! Dynamic description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || yes || [[File:rrpc1.PNG|thumb]] ||The trajectory passes through the transition state as the reaction has enough energy. The B-C bond breaks and the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2 || -100.456 || no ||[[File:RrpC2.PNG|thumb]] ||The trajectory does not pass through the activation barrier as there is not enough energy&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || yes || [[File:rrpc3.PNG|thumb]] ||The trajectory goes through the transition state as the reaction has sufficient energy to overcome the activation barrier and the B-C bond breaks whilst the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5 || -84.956 || no || [[File:rrpc4.PNG|thumb]] || The B-A bond formed however, the trajectory reverts back to the reactants and the B-C bond reforms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || yes || [[File:rrpc5.PNG|thumb]] || the B-A bond forms, only to revert back and re-form the B-C bond. Subsequently, the B-A bond forms again. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It is clear that the higher the total energy the more likely the reaction will go to completion as the energy is greater than the activation energy. However, it can be seen that with the last two contour plots, the products do not form-another variable affects the outcome of the reaction other than activation energy!&lt;br /&gt;
&lt;br /&gt;
====Assumptions of Transition State Theory====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory explains how the rate of a chemical reaction by which the reaction passes through a transition state and it has three assumptions:&lt;br /&gt;
&lt;br /&gt;
-The energy of the particles follow a Boltzmann distribution&lt;br /&gt;
-The reactants and transition state structure is in equilibrium&lt;br /&gt;
-The transition state structure does not revert back to the reactants once the reactants form the transition state&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;Exercise 2: F-H-H system&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
Using the energy surface, the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction as the products are lower in energy than the reactants.This bond breaking process must mean that the H-F bond is stronger than the H-H and this relates t the ionic nature of the bond due to the large difference in electronegativity between the atoms. Thus, the reverse reaction must be endothermic.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpf.PNG|thumb|center|Surface plot of the F-H-H system with AB=HF and BC=H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====The approximate position of the transition state====&lt;br /&gt;
&lt;br /&gt;
Using a MEP contour plot, the saddle point (where there is no momentum) was determined. AB=1.908 Å , BC=0.745 Å. The use of an internuclear distance vs time also highlighted this.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Contour Plot !! Zoom of Contour !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpts.PNG|thumb|center|Contour plot of trajectory| 250px]]  || [[File:rrpzm.PNG|thumb| Trajectory zoomed in]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Activation energy====&lt;br /&gt;
&lt;br /&gt;
The activation energy for both reactions was determined by calculating the difference between the reactants/products and the transition state using an energy vs time plot .&lt;br /&gt;
&lt;br /&gt;
-For the H + HF reaction the activation energy was found to be 30 kcal/mol. &lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction the activation energy was found to be 0.026 kcal/mol. This was determined by zooming in on the energy vs time plot: number = 5000 and the BC distance was deviated to 1.82 angstroms and the activation energy is the difference between the total and potential energies.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:rrphf.PNG|thumb|center|Finding the activation energy for the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction|250px]]&lt;br /&gt;
[[File:rrphfa.PNG|thumb|center|Finding the activation energy for the H + HF reaction|250px]]&lt;br /&gt;
&lt;br /&gt;
====Mechanism for the release of the reaction energy====&lt;br /&gt;
&lt;br /&gt;
Given that this reaction is exothermic, the thermal energy released would result in an overall increase in kinetic energy and a fall of the potential. Moreover, this exothermic reaction can be determined with calorimetry with sufficient insulation to prevent heat loss.&lt;br /&gt;
&lt;br /&gt;
The initial conditions that result in a reactive trajectory:&lt;br /&gt;
HH distance of 0.74&lt;br /&gt;
HF distance of 2.3&lt;br /&gt;
HF momentum of -2.2&lt;br /&gt;
HH momentum of -1.9&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The results are shown below and show that the potential energy is a mirror of the kinetic energy and the potential energy converts to kinetic- this is how energy is conserved.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpcons.PNG|thumb|center|Energy vs Time |250px]]&lt;br /&gt;
[[File:rrpmvt.PNG|thumb|center|Momentum vs Time |250px]]&lt;br /&gt;
&lt;br /&gt;
====Distribution of energy between different modes====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rules&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; explain that the efficiency of the reaction is affected by the distribution of energy between different modes; an exothermic reaction has an early transition state and translational energy plays a more fundamental role than vibrational energy in the efficiency of the reaction and vice versa. The r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; momentum corresponds to the vibrational energy and the r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; corresponds to the translational energy.&lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction, it can be seen using a dynamic contour plot, when translational energy is greater than vibrational energy, the reaction is efficient and is complete. This exothermic reaction follows Polanyi&#039;s rules.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Incomplete !! Complete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrph2com.PNG|thumb| High translational energy leads to a complete reaction|250px]]  || [[File:rrph2non.PNG|thumb|Low translational energy does not lead to a complete reaction|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-For the HF + F reaction, the transition state is late and vibrational energy, according to Polyani&#039;s rules, is more important than translational and allows a more efficient reaction for this endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Complete !! inComplete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpyes.PNG|thumb|High vibrational energy, reaction complete|250px]]  || [[File:rrpno.PNG|thumb|Low vibrational energy, reaction incomplete|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;References&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
[1]Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction, Zhaojun Zhang, Yong Zhou,† and Dong H. Zhang, dx.doi.org/10.1021/jz301649w | J. Phys. Chem. Lett. 2012, 3, 3416−3419&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794083</id>
		<title>Rrp17</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794083"/>
		<updated>2019-06-03T12:28:17Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* How is the transition state defined? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= &amp;lt;b&amp;gt;Molecular Reaction Dynamics &amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
= &amp;lt;b&amp;gt;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
If H collides with a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, there system can be defined as an AB and C.&lt;br /&gt;
{{{{fontcolor|pink| This is a slightly pointless statement as &amp;quot;an AB and C&amp;quot; doesn&#039;t really mean anything! Make sure you are always clear and spell everything out very explicitly, i.e. saying the atoms can be labelled... etc.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:25, 3 June 2019 (BST)}}&lt;br /&gt;
==== How is the transition state defined? ====&lt;br /&gt;
&lt;br /&gt;
The transition state is the maximum on the minimum energy path that links reactants to products; this point is where, ∂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, the gradient of the potential energy is zero and the distance r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; .  &lt;br /&gt;
&lt;br /&gt;
[[File:rrps_plot.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 1:&amp;lt;/b&amp;gt;The surface plot of the reaction between H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. The energies are represented by red and blue colours (high and low potential energy) and the black line is the trajectory of the reaction.|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
It can be seen that the transition state can be distinguished from a local minimum by plotting a tangent at the inflection point of the minimum energy path. The first derivative, ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q1&amp;lt;sub&amp;gt;q1&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;gt;0and the second derivative ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q2&amp;lt;sub&amp;gt;q2&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;lt;0&lt;br /&gt;
This would give you a maximum however, a tangent perpendicular to the q&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; would derive the minimum; this location is known as the saddle point and thus the transition state of a reaction. The transition state is a saddle point, it is where the minimum , q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and max ,q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; intersect.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Yes, great understanding shown here. Also (I can infer you already know this from your answer but it&#039;s always good to be detailed so...) on the perpendicular tangent you mention on which the TS is a minimum, the second partial derivate would be positive as it is a minimum. Also make sure you say second partial derivative not just second derivative. Otherwise good. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:28, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is symmetric and hence, 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;, the momentum are zero and there is no gradient at the ridge. The location of the transition state can can be seen in plot 2 and the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) was found to be 0.9077 Å.&lt;br /&gt;
This was determined by choosing a random value of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and changing the inter-nuclear distance until the force equalled zero. &lt;br /&gt;
&lt;br /&gt;
[[File:rrp17_i_t.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 2&amp;lt;/b&amp;gt; A plot of inter-nuclear distance vs time for the bond distance of 0.907 Å.|200px ]]&lt;br /&gt;
&lt;br /&gt;
====Minimum energy path and trajectory====&lt;br /&gt;
&lt;br /&gt;
The trajectory is a reaction path of minimum energy where the velocities/momenta are set to zero in each time step. This is where we displayed the transition state position by r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta is zero. This is shown in plot 3. &lt;br /&gt;
&lt;br /&gt;
However, MEP cannot characterise a reaction in terms of the motion of atoms. The reaction calculation under &#039;Dynamics&#039; that is shown in plot 4.&lt;br /&gt;
&lt;br /&gt;
It can be seen that the MEP plot is a plateaued line as the kinetic energy is reset to zero at every interval and, there molecules are not vibrating however, with the dynamic plot, the line is seen as oscillating as the molecules have momentum.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! MEP !! Dynamic !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:Rrpep.PNG|thumb|&amp;lt;b&amp;gt;Plot 3&amp;lt;/b&amp;gt; The MEP surface plot.|250px ]] || [[File:Rrpyn.PNG|thumb|&amp;lt;b&amp;gt;Plot 4&amp;lt;/b&amp;gt; The trajectory surface plot|250px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Reactive and nonreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ caption&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy (Kcal/mol) !! Reactive? !! Trajectory contour plot !! Dynamic description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || yes || [[File:rrpc1.PNG|thumb]] ||The trajectory passes through the transition state as the reaction has enough energy. The B-C bond breaks and the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2 || -100.456 || no ||[[File:RrpC2.PNG|thumb]] ||The trajectory does not pass through the activation barrier as there is not enough energy&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || yes || [[File:rrpc3.PNG|thumb]] ||The trajectory goes through the transition state as the reaction has sufficient energy to overcome the activation barrier and the B-C bond breaks whilst the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5 || -84.956 || no || [[File:rrpc4.PNG|thumb]] || The B-A bond formed however, the trajectory reverts back to the reactants and the B-C bond reforms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || yes || [[File:rrpc5.PNG|thumb]] || the B-A bond forms, only to revert back and re-form the B-C bond. Subsequently, the B-A bond forms again. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It is clear that the higher the total energy the more likely the reaction will go to completion as the energy is greater than the activation energy. However, it can be seen that with the last two contour plots, the products do not form-another variable affects the outcome of the reaction other than activation energy!&lt;br /&gt;
&lt;br /&gt;
====Assumptions of Transition State Theory====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory explains how the rate of a chemical reaction by which the reaction passes through a transition state and it has three assumptions:&lt;br /&gt;
&lt;br /&gt;
-The energy of the particles follow a Boltzmann distribution&lt;br /&gt;
-The reactants and transition state structure is in equilibrium&lt;br /&gt;
-The transition state structure does not revert back to the reactants once the reactants form the transition state&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;Exercise 2: F-H-H system&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
Using the energy surface, the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction as the products are lower in energy than the reactants.This bond breaking process must mean that the H-F bond is stronger than the H-H and this relates t the ionic nature of the bond due to the large difference in electronegativity between the atoms. Thus, the reverse reaction must be endothermic.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpf.PNG|thumb|center|Surface plot of the F-H-H system with AB=HF and BC=H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====The approximate position of the transition state====&lt;br /&gt;
&lt;br /&gt;
Using a MEP contour plot, the saddle point (where there is no momentum) was determined. AB=1.908 Å , BC=0.745 Å. The use of an internuclear distance vs time also highlighted this.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Contour Plot !! Zoom of Contour !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpts.PNG|thumb|center|Contour plot of trajectory| 250px]]  || [[File:rrpzm.PNG|thumb| Trajectory zoomed in]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Activation energy====&lt;br /&gt;
&lt;br /&gt;
The activation energy for both reactions was determined by calculating the difference between the reactants/products and the transition state using an energy vs time plot .&lt;br /&gt;
&lt;br /&gt;
-For the H + HF reaction the activation energy was found to be 30 kcal/mol. &lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction the activation energy was found to be 0.026 kcal/mol. This was determined by zooming in on the energy vs time plot: number = 5000 and the BC distance was deviated to 1.82 angstroms and the activation energy is the difference between the total and potential energies.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:rrphf.PNG|thumb|center|Finding the activation energy for the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction|250px]]&lt;br /&gt;
[[File:rrphfa.PNG|thumb|center|Finding the activation energy for the H + HF reaction|250px]]&lt;br /&gt;
&lt;br /&gt;
====Mechanism for the release of the reaction energy====&lt;br /&gt;
&lt;br /&gt;
Given that this reaction is exothermic, the thermal energy released would result in an overall increase in kinetic energy and a fall of the potential. Moreover, this exothermic reaction can be determined with calorimetry with sufficient insulation to prevent heat loss.&lt;br /&gt;
&lt;br /&gt;
The initial conditions that result in a reactive trajectory:&lt;br /&gt;
HH distance of 0.74&lt;br /&gt;
HF distance of 2.3&lt;br /&gt;
HF momentum of -2.2&lt;br /&gt;
HH momentum of -1.9&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The results are shown below and show that the potential energy is a mirror of the kinetic energy and the potential energy converts to kinetic- this is how energy is conserved.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpcons.PNG|thumb|center|Energy vs Time |250px]]&lt;br /&gt;
[[File:rrpmvt.PNG|thumb|center|Momentum vs Time |250px]]&lt;br /&gt;
&lt;br /&gt;
====Distribution of energy between different modes====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rules&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; explain that the efficiency of the reaction is affected by the distribution of energy between different modes; an exothermic reaction has an early transition state and translational energy plays a more fundamental role than vibrational energy in the efficiency of the reaction and vice versa. The r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; momentum corresponds to the vibrational energy and the r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; corresponds to the translational energy.&lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction, it can be seen using a dynamic contour plot, when translational energy is greater than vibrational energy, the reaction is efficient and is complete. This exothermic reaction follows Polanyi&#039;s rules.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Incomplete !! Complete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrph2com.PNG|thumb| High translational energy leads to a complete reaction|250px]]  || [[File:rrph2non.PNG|thumb|Low translational energy does not lead to a complete reaction|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-For the HF + F reaction, the transition state is late and vibrational energy, according to Polyani&#039;s rules, is more important than translational and allows a more efficient reaction for this endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Complete !! inComplete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpyes.PNG|thumb|High vibrational energy, reaction complete|250px]]  || [[File:rrpno.PNG|thumb|Low vibrational energy, reaction incomplete|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;References&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
[1]Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction, Zhaojun Zhang, Yong Zhou,† and Dong H. Zhang, dx.doi.org/10.1021/jz301649w | J. Phys. Chem. Lett. 2012, 3, 3416−3419&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794082</id>
		<title>Rrp17</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794082"/>
		<updated>2019-06-03T12:28:05Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* How is the transition state defined? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= &amp;lt;b&amp;gt;Molecular Reaction Dynamics &amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
= &amp;lt;b&amp;gt;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
If H collides with a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, there system can be defined as an AB and C.&lt;br /&gt;
{{{{fontcolor|pink| This is a slightly pointless statement as &amp;quot;an AB and C&amp;quot; doesn&#039;t really mean anything! Make sure you are always clear and spell everything out very explicitly, i.e. saying the atoms can be labelled... etc.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:25, 3 June 2019 (BST)}}&lt;br /&gt;
==== How is the transition state defined? ====&lt;br /&gt;
&lt;br /&gt;
The transition state is the maximum on the minimum energy path that links reactants to products; this point is where, ∂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, the gradient of the potential energy is zero and the distance r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; .  &lt;br /&gt;
&lt;br /&gt;
[[File:rrps_plot.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 1:&amp;lt;/b&amp;gt;The surface plot of the reaction between H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. The energies are represented by red and blue colours (high and low potential energy) and the black line is the trajectory of the reaction.|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
It can be seen that the transition state can be distinguished from a local minimum by plotting a tangent at the inflection point of the minimum energy path. The first derivative, ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q1&amp;lt;sub&amp;gt;q1&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;gt;0and the second derivative ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q2&amp;lt;sub&amp;gt;q2&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;lt;0&lt;br /&gt;
This would give you a maximum however, a tangent perpendicular to the q&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; would derive the minimum; this location is known as the saddle point and thus the transition state of a reaction. The transition state is a saddle point, it is where the minimum , q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and max ,q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; intersect.&lt;br /&gt;
&lt;br /&gt;
{{{{fontcolor|pink|Yes, great understanding shown here. Also (I can infer you already know this from your answer but it&#039;s always good to be detailed so...) on the perpendicular tangent you mention on which the TS is a minimum, the second partial derivate would be positive as it is a minimum. Also make sure you say second partial derivative not just second derivative. Otherwise good. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:28, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is symmetric and hence, 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;, the momentum are zero and there is no gradient at the ridge. The location of the transition state can can be seen in plot 2 and the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) was found to be 0.9077 Å.&lt;br /&gt;
This was determined by choosing a random value of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and changing the inter-nuclear distance until the force equalled zero. &lt;br /&gt;
&lt;br /&gt;
[[File:rrp17_i_t.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 2&amp;lt;/b&amp;gt; A plot of inter-nuclear distance vs time for the bond distance of 0.907 Å.|200px ]]&lt;br /&gt;
&lt;br /&gt;
====Minimum energy path and trajectory====&lt;br /&gt;
&lt;br /&gt;
The trajectory is a reaction path of minimum energy where the velocities/momenta are set to zero in each time step. This is where we displayed the transition state position by r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta is zero. This is shown in plot 3. &lt;br /&gt;
&lt;br /&gt;
However, MEP cannot characterise a reaction in terms of the motion of atoms. The reaction calculation under &#039;Dynamics&#039; that is shown in plot 4.&lt;br /&gt;
&lt;br /&gt;
It can be seen that the MEP plot is a plateaued line as the kinetic energy is reset to zero at every interval and, there molecules are not vibrating however, with the dynamic plot, the line is seen as oscillating as the molecules have momentum.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! MEP !! Dynamic !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:Rrpep.PNG|thumb|&amp;lt;b&amp;gt;Plot 3&amp;lt;/b&amp;gt; The MEP surface plot.|250px ]] || [[File:Rrpyn.PNG|thumb|&amp;lt;b&amp;gt;Plot 4&amp;lt;/b&amp;gt; The trajectory surface plot|250px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Reactive and nonreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ caption&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy (Kcal/mol) !! Reactive? !! Trajectory contour plot !! Dynamic description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || yes || [[File:rrpc1.PNG|thumb]] ||The trajectory passes through the transition state as the reaction has enough energy. The B-C bond breaks and the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2 || -100.456 || no ||[[File:RrpC2.PNG|thumb]] ||The trajectory does not pass through the activation barrier as there is not enough energy&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || yes || [[File:rrpc3.PNG|thumb]] ||The trajectory goes through the transition state as the reaction has sufficient energy to overcome the activation barrier and the B-C bond breaks whilst the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5 || -84.956 || no || [[File:rrpc4.PNG|thumb]] || The B-A bond formed however, the trajectory reverts back to the reactants and the B-C bond reforms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || yes || [[File:rrpc5.PNG|thumb]] || the B-A bond forms, only to revert back and re-form the B-C bond. Subsequently, the B-A bond forms again. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It is clear that the higher the total energy the more likely the reaction will go to completion as the energy is greater than the activation energy. However, it can be seen that with the last two contour plots, the products do not form-another variable affects the outcome of the reaction other than activation energy!&lt;br /&gt;
&lt;br /&gt;
====Assumptions of Transition State Theory====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory explains how the rate of a chemical reaction by which the reaction passes through a transition state and it has three assumptions:&lt;br /&gt;
&lt;br /&gt;
-The energy of the particles follow a Boltzmann distribution&lt;br /&gt;
-The reactants and transition state structure is in equilibrium&lt;br /&gt;
-The transition state structure does not revert back to the reactants once the reactants form the transition state&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;Exercise 2: F-H-H system&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
Using the energy surface, the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction as the products are lower in energy than the reactants.This bond breaking process must mean that the H-F bond is stronger than the H-H and this relates t the ionic nature of the bond due to the large difference in electronegativity between the atoms. Thus, the reverse reaction must be endothermic.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpf.PNG|thumb|center|Surface plot of the F-H-H system with AB=HF and BC=H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====The approximate position of the transition state====&lt;br /&gt;
&lt;br /&gt;
Using a MEP contour plot, the saddle point (where there is no momentum) was determined. AB=1.908 Å , BC=0.745 Å. The use of an internuclear distance vs time also highlighted this.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Contour Plot !! Zoom of Contour !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpts.PNG|thumb|center|Contour plot of trajectory| 250px]]  || [[File:rrpzm.PNG|thumb| Trajectory zoomed in]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Activation energy====&lt;br /&gt;
&lt;br /&gt;
The activation energy for both reactions was determined by calculating the difference between the reactants/products and the transition state using an energy vs time plot .&lt;br /&gt;
&lt;br /&gt;
-For the H + HF reaction the activation energy was found to be 30 kcal/mol. &lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction the activation energy was found to be 0.026 kcal/mol. This was determined by zooming in on the energy vs time plot: number = 5000 and the BC distance was deviated to 1.82 angstroms and the activation energy is the difference between the total and potential energies.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:rrphf.PNG|thumb|center|Finding the activation energy for the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction|250px]]&lt;br /&gt;
[[File:rrphfa.PNG|thumb|center|Finding the activation energy for the H + HF reaction|250px]]&lt;br /&gt;
&lt;br /&gt;
====Mechanism for the release of the reaction energy====&lt;br /&gt;
&lt;br /&gt;
Given that this reaction is exothermic, the thermal energy released would result in an overall increase in kinetic energy and a fall of the potential. Moreover, this exothermic reaction can be determined with calorimetry with sufficient insulation to prevent heat loss.&lt;br /&gt;
&lt;br /&gt;
The initial conditions that result in a reactive trajectory:&lt;br /&gt;
HH distance of 0.74&lt;br /&gt;
HF distance of 2.3&lt;br /&gt;
HF momentum of -2.2&lt;br /&gt;
HH momentum of -1.9&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The results are shown below and show that the potential energy is a mirror of the kinetic energy and the potential energy converts to kinetic- this is how energy is conserved.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpcons.PNG|thumb|center|Energy vs Time |250px]]&lt;br /&gt;
[[File:rrpmvt.PNG|thumb|center|Momentum vs Time |250px]]&lt;br /&gt;
&lt;br /&gt;
====Distribution of energy between different modes====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rules&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; explain that the efficiency of the reaction is affected by the distribution of energy between different modes; an exothermic reaction has an early transition state and translational energy plays a more fundamental role than vibrational energy in the efficiency of the reaction and vice versa. The r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; momentum corresponds to the vibrational energy and the r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; corresponds to the translational energy.&lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction, it can be seen using a dynamic contour plot, when translational energy is greater than vibrational energy, the reaction is efficient and is complete. This exothermic reaction follows Polanyi&#039;s rules.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Incomplete !! Complete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrph2com.PNG|thumb| High translational energy leads to a complete reaction|250px]]  || [[File:rrph2non.PNG|thumb|Low translational energy does not lead to a complete reaction|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-For the HF + F reaction, the transition state is late and vibrational energy, according to Polyani&#039;s rules, is more important than translational and allows a more efficient reaction for this endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Complete !! inComplete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpyes.PNG|thumb|High vibrational energy, reaction complete|250px]]  || [[File:rrpno.PNG|thumb|Low vibrational energy, reaction incomplete|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;References&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
[1]Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction, Zhaojun Zhang, Yong Zhou,† and Dong H. Zhang, dx.doi.org/10.1021/jz301649w | J. Phys. Chem. Lett. 2012, 3, 3416−3419&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794081</id>
		<title>Rrp17</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rrp17&amp;diff=794081"/>
		<updated>2019-06-03T12:25:54Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* EXERCISE 1: H + H2 system */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= &amp;lt;b&amp;gt;Molecular Reaction Dynamics &amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
= &amp;lt;b&amp;gt;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&amp;lt;/b&amp;gt; =&lt;br /&gt;
&lt;br /&gt;
If H collides with a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, there system can be defined as an AB and C.&lt;br /&gt;
{{{{fontcolor|pink| This is a slightly pointless statement as &amp;quot;an AB and C&amp;quot; doesn&#039;t really mean anything! Make sure you are always clear and spell everything out very explicitly, i.e. saying the atoms can be labelled... etc.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:25, 3 June 2019 (BST)}}&lt;br /&gt;
==== How is the transition state defined? ====&lt;br /&gt;
&lt;br /&gt;
The transition state is the maximum on the minimum energy path that links reactants to products; this point is where, ∂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, the gradient of the potential energy is zero and the distance r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; .  &lt;br /&gt;
&lt;br /&gt;
[[File:rrps_plot.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 1:&amp;lt;/b&amp;gt;The surface plot of the reaction between H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. The energies are represented by red and blue colours (high and low potential energy) and the black line is the trajectory of the reaction.|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
It can be seen that the transition state can be distinguished from a local minimum by plotting a tangent at the inflection point of the minimum energy path. The first derivative, ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q1&amp;lt;sub&amp;gt;q1&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;gt;0and the second derivative ∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/∂q2&amp;lt;sub&amp;gt;q2&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;&amp;lt;0&lt;br /&gt;
This would give you a maximum however, a tangent perpendicular to the q&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; would derive the minimum; this location is known as the saddle point and thus the transition state of a reaction. The transition state is a saddle point, it is where the minimum , q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and max ,q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; intersect.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is symmetric and hence, 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;, the momentum are zero and there is no gradient at the ridge. The location of the transition state can can be seen in plot 2 and the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) was found to be 0.9077 Å.&lt;br /&gt;
This was determined by choosing a random value of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and changing the inter-nuclear distance until the force equalled zero. &lt;br /&gt;
&lt;br /&gt;
[[File:rrp17_i_t.PNG|thumb|center|&amp;lt;b&amp;gt;Plot 2&amp;lt;/b&amp;gt; A plot of inter-nuclear distance vs time for the bond distance of 0.907 Å.|200px ]]&lt;br /&gt;
&lt;br /&gt;
====Minimum energy path and trajectory====&lt;br /&gt;
&lt;br /&gt;
The trajectory is a reaction path of minimum energy where the velocities/momenta are set to zero in each time step. This is where we displayed the transition state position by r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta is zero. This is shown in plot 3. &lt;br /&gt;
&lt;br /&gt;
However, MEP cannot characterise a reaction in terms of the motion of atoms. The reaction calculation under &#039;Dynamics&#039; that is shown in plot 4.&lt;br /&gt;
&lt;br /&gt;
It can be seen that the MEP plot is a plateaued line as the kinetic energy is reset to zero at every interval and, there molecules are not vibrating however, with the dynamic plot, the line is seen as oscillating as the molecules have momentum.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! MEP !! Dynamic !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:Rrpep.PNG|thumb|&amp;lt;b&amp;gt;Plot 3&amp;lt;/b&amp;gt; The MEP surface plot.|250px ]] || [[File:Rrpyn.PNG|thumb|&amp;lt;b&amp;gt;Plot 4&amp;lt;/b&amp;gt; The trajectory surface plot|250px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Reactive and nonreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ caption&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy (Kcal/mol) !! Reactive? !! Trajectory contour plot !! Dynamic description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || yes || [[File:rrpc1.PNG|thumb]] ||The trajectory passes through the transition state as the reaction has enough energy. The B-C bond breaks and the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2 || -100.456 || no ||[[File:RrpC2.PNG|thumb]] ||The trajectory does not pass through the activation barrier as there is not enough energy&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || yes || [[File:rrpc3.PNG|thumb]] ||The trajectory goes through the transition state as the reaction has sufficient energy to overcome the activation barrier and the B-C bond breaks whilst the A-B bond forms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5 || -84.956 || no || [[File:rrpc4.PNG|thumb]] || The B-A bond formed however, the trajectory reverts back to the reactants and the B-C bond reforms.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || yes || [[File:rrpc5.PNG|thumb]] || the B-A bond forms, only to revert back and re-form the B-C bond. Subsequently, the B-A bond forms again. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It is clear that the higher the total energy the more likely the reaction will go to completion as the energy is greater than the activation energy. However, it can be seen that with the last two contour plots, the products do not form-another variable affects the outcome of the reaction other than activation energy!&lt;br /&gt;
&lt;br /&gt;
====Assumptions of Transition State Theory====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory explains how the rate of a chemical reaction by which the reaction passes through a transition state and it has three assumptions:&lt;br /&gt;
&lt;br /&gt;
-The energy of the particles follow a Boltzmann distribution&lt;br /&gt;
-The reactants and transition state structure is in equilibrium&lt;br /&gt;
-The transition state structure does not revert back to the reactants once the reactants form the transition state&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;Exercise 2: F-H-H system&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
Using the energy surface, the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction as the products are lower in energy than the reactants.This bond breaking process must mean that the H-F bond is stronger than the H-H and this relates t the ionic nature of the bond due to the large difference in electronegativity between the atoms. Thus, the reverse reaction must be endothermic.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpf.PNG|thumb|center|Surface plot of the F-H-H system with AB=HF and BC=H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;|250px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
====The approximate position of the transition state====&lt;br /&gt;
&lt;br /&gt;
Using a MEP contour plot, the saddle point (where there is no momentum) was determined. AB=1.908 Å , BC=0.745 Å. The use of an internuclear distance vs time also highlighted this.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Contour Plot !! Zoom of Contour !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpts.PNG|thumb|center|Contour plot of trajectory| 250px]]  || [[File:rrpzm.PNG|thumb| Trajectory zoomed in]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====Activation energy====&lt;br /&gt;
&lt;br /&gt;
The activation energy for both reactions was determined by calculating the difference between the reactants/products and the transition state using an energy vs time plot .&lt;br /&gt;
&lt;br /&gt;
-For the H + HF reaction the activation energy was found to be 30 kcal/mol. &lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction the activation energy was found to be 0.026 kcal/mol. This was determined by zooming in on the energy vs time plot: number = 5000 and the BC distance was deviated to 1.82 angstroms and the activation energy is the difference between the total and potential energies.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:rrphf.PNG|thumb|center|Finding the activation energy for the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction|250px]]&lt;br /&gt;
[[File:rrphfa.PNG|thumb|center|Finding the activation energy for the H + HF reaction|250px]]&lt;br /&gt;
&lt;br /&gt;
====Mechanism for the release of the reaction energy====&lt;br /&gt;
&lt;br /&gt;
Given that this reaction is exothermic, the thermal energy released would result in an overall increase in kinetic energy and a fall of the potential. Moreover, this exothermic reaction can be determined with calorimetry with sufficient insulation to prevent heat loss.&lt;br /&gt;
&lt;br /&gt;
The initial conditions that result in a reactive trajectory:&lt;br /&gt;
HH distance of 0.74&lt;br /&gt;
HF distance of 2.3&lt;br /&gt;
HF momentum of -2.2&lt;br /&gt;
HH momentum of -1.9&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The results are shown below and show that the potential energy is a mirror of the kinetic energy and the potential energy converts to kinetic- this is how energy is conserved.&lt;br /&gt;
&lt;br /&gt;
[[File:rrpcons.PNG|thumb|center|Energy vs Time |250px]]&lt;br /&gt;
[[File:rrpmvt.PNG|thumb|center|Momentum vs Time |250px]]&lt;br /&gt;
&lt;br /&gt;
====Distribution of energy between different modes====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rules&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt; explain that the efficiency of the reaction is affected by the distribution of energy between different modes; an exothermic reaction has an early transition state and translational energy plays a more fundamental role than vibrational energy in the efficiency of the reaction and vice versa. The r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; momentum corresponds to the vibrational energy and the r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; corresponds to the translational energy.&lt;br /&gt;
&lt;br /&gt;
-For the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F reaction, it can be seen using a dynamic contour plot, when translational energy is greater than vibrational energy, the reaction is efficient and is complete. This exothermic reaction follows Polanyi&#039;s rules.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Incomplete !! Complete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrph2com.PNG|thumb| High translational energy leads to a complete reaction|250px]]  || [[File:rrph2non.PNG|thumb|Low translational energy does not lead to a complete reaction|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-For the HF + F reaction, the transition state is late and vibrational energy, according to Polyani&#039;s rules, is more important than translational and allows a more efficient reaction for this endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Complete !! inComplete !!  &lt;br /&gt;
|-&lt;br /&gt;
| [[File:rrpyes.PNG|thumb|High vibrational energy, reaction complete|250px]]  || [[File:rrpno.PNG|thumb|Low vibrational energy, reaction incomplete|250px]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=&amp;lt;b&amp;gt;References&amp;lt;/b&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
[1]Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction, Zhaojun Zhang, Yong Zhou,† and Dong H. Zhang, dx.doi.org/10.1021/jz301649w | J. Phys. Chem. Lett. 2012, 3, 3416−3419&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794080</id>
		<title>013366322</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794080"/>
		<updated>2019-06-03T12:24:22Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Q9 - 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&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system  ==&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q1 - 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?&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
On the potential energy surface, the transition state is the position along the minimum energy pathway, linking reactants and products, where potential is highest. The transition structure exists at a saddle point of the potential energy surface - that is when ∂V(&#039;&#039;&#039;ri&#039;&#039;&#039;)/∂(&#039;&#039;&#039;ri&#039;&#039;&#039;)=0. Furthermore, the 2nd partial derivatives with respect to the orthogonal vectors r1 and r2 have opposite signs; one is positive and the other negative. This tells us that this is a saddle point.&lt;br /&gt;
&lt;br /&gt;
[[File:Screenshot_2019-05-21_at_14.27.22.png|400px]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Be careful to makesure you say &amp;quot;potential energy&amp;quot; not just &amp;quot;potential&amp;quot;. And yes this is all correct and clearly explained but you are missing part of the definition. The TS is a saddle point because it is the maximum along the reaction trajectory and a minimum in the orthogonal direction, so which vector r1 or r2 will be positive or negative? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:47, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q2 - 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.&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 14.41.20.png|thumb|upright|400x400px|A graph showing Intermolecular distance Vs Time ]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_16.25.22.png|thumb|upright|400x400px|Contour Plot to find rts]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Firstly, we set AB=BC and momentum equal to 0. Then, plotting a graph of Internuclear Distance vs Time, we can find the transition state. The optimised distance is the distance at which there is no trajectory towards either reactants or products and at which oscillations are reduced producing a straight line as seen in the plot above. As the graph shows straight lines, we know there is no vibration, and the atoms stop moving. That is, potential energy is maximum and kinetic energy zero. As such, the optimised distance is found to be 0.9079 Å. Looking at the contour plot above, the transition state can also be seen in approximately the correct location, backing up the result.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Great explanation - very clear and well understood.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:50, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q3 - Comment on how the MEP and the trajectory you just calculated differ.&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_15.06.08.png|thumb|upright|400x400px|MEP Calculation]]&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 15.07.56.png|thumb|upright|400x400px|Dynamics Calculation]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The MEP graph shows no molecular vibration (as velocity=0) with momentum being equal to 0 in every time step. In comparison, the dynamics plot shows the vibrational energy of the molecule as seen by the non-straight line.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|True, can you think of why? In terms of the calculation process itself? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:54, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q4 - 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?&#039;&#039;&#039;===&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; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the trajectory !! Description of the dynamics &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || YES || [[File:Screenshot_dex_1.png|400x400px]] || Both reactants collide and have sufficient energy to surpass the activation barrier. Products are formed. Vibrational motion is also seen evident by the oscillations.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0  || -100.456 || NO || [[File:Screenshot_dex_2.png|400x400px]] || Atom C collides molecule AB but has insufficient kinetic energy to overcome the activation energy, thus not forming products. Molecules do not pass through the transition state.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5  || -98.956 || YES || [[File:Screenshot_dex_3.png|400x400px]] || Both molecules have sufficient energy to surpass the activation energy and so pass though the transition state, forming the products.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0  || -84.956 || NO || [[File:Screenshot_dex_4.png|400x400px]] || Both molecules have large energies and are able to overcome the activation energy. However, their energy is so great, that they recross the barrier and reform reactants.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2  || -83.416 || YES || [[File:Screenshot_dex_5.png|400x400px]] || Both molecules have sufficient energy to overcome the activation energy barrier, but have the potential to cross back over the barrier, and reform products. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It can be concluded that if reactants do not have sufficient kinetic energy to surpass the activation barrier, then the reaction will not occur. Furthermore, if the reactants have an excess of kinetic energy, the reaction also may not proceed as the products formed turn back into reactants.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Yes, or you could also say that there is not a simple threshold energy to determine whether or not the system will be reactive. It is not as simple as molecules that do have the activation energy will react, and molecules that don&#039;t won&#039;t react. That would be the simplest form of conclusion to be drawn from this. Your observations are clear and insightful. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:59, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q5 - State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Electron and nuclear motion are independent&lt;br /&gt;
Energy of the particles follows the Boltzmann distribution&lt;br /&gt;
Once reactants begin to combine and form the transition state, the transition state structure does not collapse to form reactants again&lt;br /&gt;
&lt;br /&gt;
Theory states that transition state structure does not collapse to reform the reactants. However, as experimental procedure shows, this can occur. As theory assumes that all reactions with sufficient energy will go onto form products, the real rate of reaction is much slower than in theory as reactants can be reformed.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Great![[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:00, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== EXERCISE 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q6 - 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?&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
 {|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_dex_f_h2.png|thumb|upright|400x400px|Surface Plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_dex_h_hf.png|thumb|upright|400x400px|Surface Plot for H + HF]]&lt;br /&gt;
|}&lt;br /&gt;
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As seen above, the surface plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; starts at a high energy position dropping down lower energy after the transition state. Therefore, this is an exothermic reaction. In contrast, for the surface plot of HF + H, the reaction starts at a low energy position and needs a large amount of energy to over come the activation energy barrier. After passing the transition state, the energy falls a small amount. This reaction is therefore endothermic. From this, we can conclude that the HF bond is stronger than the HH bond since HF is lower in energy than HH. &lt;br /&gt;
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Furthermore, Hammond&#039;s Postulate states that the transition state will resemble either the product or reactants, whichever it is closer to in energy. To find the transition state, optimisation was completed as before with both momenta set to zero. Optimisation was completed so that there was minimal oscillation (gradient of line =0) seen for the Internuclear Distance vs Time graph, as shown below. The optimised distances were found to be r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-F)=1.813 Å and r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-H)=0.7445 Å. &lt;br /&gt;
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[[File:Screenshot_2019-05-21_at_18.21.10.png|thumb|upright|400x400px|Graph showing Internuclear Distance vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
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===&#039;&#039;&#039;Q7 - Report the activation energy for both reactions.&#039;&#039;&#039;===&lt;br /&gt;
Below shows two graphs depicting the total energy plot of both reactions. The activation energy for both reactions can be calculated as the difference between the highest and lowest energy levels. &lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.37.01.png|500px|left|thumb|Graph of Energy vs Steps for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.41.09.png|500px|right|thumb|Graph of Energy vs Steps for HF + H.]]&lt;br /&gt;
|}&lt;br /&gt;
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&#039;&#039;&#039;Activation Energy(H + HF)&#039;&#039;&#039;= +31.22 kcalmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)&#039;&#039;&#039;= +0.130 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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{{fontcolor|pink|All correct and clearly presented with appropriate diagrams. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:01, 3 June 2019 (BST)}}&lt;br /&gt;
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===&#039;&#039;&#039;Q8 - 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.&#039;&#039;&#039;===&lt;br /&gt;
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For the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; a reactive trajectory was found using the following set of initial conditions: AB = 0.74 Å, BC = 1.80 Å, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5, and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.70. Using these intial conditions the graph of Momentum vs Time was produced, as seen below.&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.01.png|thumb|upright|400x400px|Graph of Momentum vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.11.png|thumb|upright|400x400px|Graph of Energy vs Time ]]&lt;br /&gt;
|}&lt;br /&gt;
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As you can see, whenever potential energy is lost, kinetic energy is gained by the same amount. Due to the exothermic nature of this reactrion, this kinetic energy is then converted into heat and can experimentally be seen by the increase in temperature.&lt;br /&gt;
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{{fontcolor|pink|Yes, that&#039;s right, can you think of a particular experimental setup/technique which can detect such a change in conditions accurately?[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:02, 3 June 2019 (BST)}}&lt;br /&gt;
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===&#039;&#039;&#039;Q9 - 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.&#039;&#039;&#039;===&lt;br /&gt;
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Polanyi&#039;s Rule states that vibrational energy is much less successful in promoting an early transition state than translational energy is. Additionally, the opposite is true - translational energy is more efficient in promoting a late transition state than vibrational energy.&lt;br /&gt;
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As seen above when calculating the activation energy of reaction, the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Hammond&#039;s Postulate states that this reaction therefore has an early transition state. Using Polanyi&#039;s Rules, this reaction would be most effectively activated by translational energy. Similarly, for the reaction of H + HF (endothermic), this would be most efficiently activated by vibrational energy.&lt;br /&gt;
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For the first reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, I used the values of r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.74 Å, and r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=1.81 Å.  Then i looked at the contour plots for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-2.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-0.5 (Left diagram), and for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-2.5 (right diagram). For the initial set of conditions, there is greater vibrational energy, and the 2nd set of conditions, greater translational energy. &lt;br /&gt;
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According to Polanyi&#039;s Rules, we would expect this reaction to be best activated by vibrational energy. The two graphs below agree with these findings. &lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.32.46.png|thumb|upright|330x330px|Contour plot for greater vibrational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.33.04.png|thumb|upright|330x330px|Contour plot for greater translational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
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{{fontcolor|pink|I don&#039;t know whether I am just not managing to clearly decipher your figure, but the left diagram doesn&#039;t look reactive to me and the right one does. You haven&#039;t done any calculations wrong but you&#039;ve mixed up your order of Polanyi&#039;s rules. In an early barrier reaction, kinetic energy is effective in overcoming the barrier but vibrational energy is ineffective in overcoming the barrier. The distinction between the two systems would be clearer if you had one with high vibrational energy and low kinetic and vice versa. These both look like they have quite high vibrational energy. Also, TST and Polanyi&#039;s rules should both be quoted with an accompanying literature reference. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:10, 3 June 2019 (BST)}}&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794079</id>
		<title>013366322</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794079"/>
		<updated>2019-06-03T12:10:16Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Q9 - 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;
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&lt;div&gt;== EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system  ==&lt;br /&gt;
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====&#039;&#039;&#039;Q1 - 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?&#039;&#039;&#039;====&lt;br /&gt;
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On the potential energy surface, the transition state is the position along the minimum energy pathway, linking reactants and products, where potential is highest. The transition structure exists at a saddle point of the potential energy surface - that is when ∂V(&#039;&#039;&#039;ri&#039;&#039;&#039;)/∂(&#039;&#039;&#039;ri&#039;&#039;&#039;)=0. Furthermore, the 2nd partial derivatives with respect to the orthogonal vectors r1 and r2 have opposite signs; one is positive and the other negative. This tells us that this is a saddle point.&lt;br /&gt;
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[[File:Screenshot_2019-05-21_at_14.27.22.png|400px]]&lt;br /&gt;
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{{fontcolor|pink|Be careful to makesure you say &amp;quot;potential energy&amp;quot; not just &amp;quot;potential&amp;quot;. And yes this is all correct and clearly explained but you are missing part of the definition. The TS is a saddle point because it is the maximum along the reaction trajectory and a minimum in the orthogonal direction, so which vector r1 or r2 will be positive or negative? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:47, 3 June 2019 (BST)}}&lt;br /&gt;
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====&#039;&#039;&#039;Q2 - 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.&#039;&#039;&#039;====&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 14.41.20.png|thumb|upright|400x400px|A graph showing Intermolecular distance Vs Time ]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_16.25.22.png|thumb|upright|400x400px|Contour Plot to find rts]]&lt;br /&gt;
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Firstly, we set AB=BC and momentum equal to 0. Then, plotting a graph of Internuclear Distance vs Time, we can find the transition state. The optimised distance is the distance at which there is no trajectory towards either reactants or products and at which oscillations are reduced producing a straight line as seen in the plot above. As the graph shows straight lines, we know there is no vibration, and the atoms stop moving. That is, potential energy is maximum and kinetic energy zero. As such, the optimised distance is found to be 0.9079 Å. Looking at the contour plot above, the transition state can also be seen in approximately the correct location, backing up the result.&lt;br /&gt;
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{{fontcolor|pink|Great explanation - very clear and well understood.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:50, 3 June 2019 (BST)}}&lt;br /&gt;
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====&#039;&#039;&#039;Q3 - Comment on how the MEP and the trajectory you just calculated differ.&#039;&#039;&#039;====&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_15.06.08.png|thumb|upright|400x400px|MEP Calculation]]&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 15.07.56.png|thumb|upright|400x400px|Dynamics Calculation]]&lt;br /&gt;
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The MEP graph shows no molecular vibration (as velocity=0) with momentum being equal to 0 in every time step. In comparison, the dynamics plot shows the vibrational energy of the molecule as seen by the non-straight line.&lt;br /&gt;
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{{fontcolor|pink|True, can you think of why? In terms of the calculation process itself? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:54, 3 June 2019 (BST)}}&lt;br /&gt;
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===&#039;&#039;&#039;Q4 - 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?&#039;&#039;&#039;===&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; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the trajectory !! Description of the dynamics &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || YES || [[File:Screenshot_dex_1.png|400x400px]] || Both reactants collide and have sufficient energy to surpass the activation barrier. Products are formed. Vibrational motion is also seen evident by the oscillations.&lt;br /&gt;
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| -1.5 || -2.0  || -100.456 || NO || [[File:Screenshot_dex_2.png|400x400px]] || Atom C collides molecule AB but has insufficient kinetic energy to overcome the activation energy, thus not forming products. Molecules do not pass through the transition state.&lt;br /&gt;
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| -1.5 || -2.5  || -98.956 || YES || [[File:Screenshot_dex_3.png|400x400px]] || Both molecules have sufficient energy to surpass the activation energy and so pass though the transition state, forming the products.&lt;br /&gt;
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| -2.5 || -5.0  || -84.956 || NO || [[File:Screenshot_dex_4.png|400x400px]] || Both molecules have large energies and are able to overcome the activation energy. However, their energy is so great, that they recross the barrier and reform reactants.&lt;br /&gt;
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| -2.5 || -5.2  || -83.416 || YES || [[File:Screenshot_dex_5.png|400x400px]] || Both molecules have sufficient energy to overcome the activation energy barrier, but have the potential to cross back over the barrier, and reform products. &lt;br /&gt;
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It can be concluded that if reactants do not have sufficient kinetic energy to surpass the activation barrier, then the reaction will not occur. Furthermore, if the reactants have an excess of kinetic energy, the reaction also may not proceed as the products formed turn back into reactants.&lt;br /&gt;
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{{fontcolor|pink|Yes, or you could also say that there is not a simple threshold energy to determine whether or not the system will be reactive. It is not as simple as molecules that do have the activation energy will react, and molecules that don&#039;t won&#039;t react. That would be the simplest form of conclusion to be drawn from this. Your observations are clear and insightful. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:59, 3 June 2019 (BST)}}&lt;br /&gt;
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===&#039;&#039;&#039;Q5 - State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;===&lt;br /&gt;
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Electron and nuclear motion are independent&lt;br /&gt;
Energy of the particles follows the Boltzmann distribution&lt;br /&gt;
Once reactants begin to combine and form the transition state, the transition state structure does not collapse to form reactants again&lt;br /&gt;
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Theory states that transition state structure does not collapse to reform the reactants. However, as experimental procedure shows, this can occur. As theory assumes that all reactions with sufficient energy will go onto form products, the real rate of reaction is much slower than in theory as reactants can be reformed.&lt;br /&gt;
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{{fontcolor|pink| Great![[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:00, 3 June 2019 (BST)}}&lt;br /&gt;
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== EXERCISE 2: F - H - H system ==&lt;br /&gt;
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===&#039;&#039;&#039;Q6 - 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?&#039;&#039;&#039;===&lt;br /&gt;
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 {|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_dex_f_h2.png|thumb|upright|400x400px|Surface Plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_dex_h_hf.png|thumb|upright|400x400px|Surface Plot for H + HF]]&lt;br /&gt;
|}&lt;br /&gt;
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As seen above, the surface plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; starts at a high energy position dropping down lower energy after the transition state. Therefore, this is an exothermic reaction. In contrast, for the surface plot of HF + H, the reaction starts at a low energy position and needs a large amount of energy to over come the activation energy barrier. After passing the transition state, the energy falls a small amount. This reaction is therefore endothermic. From this, we can conclude that the HF bond is stronger than the HH bond since HF is lower in energy than HH. &lt;br /&gt;
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Furthermore, Hammond&#039;s Postulate states that the transition state will resemble either the product or reactants, whichever it is closer to in energy. To find the transition state, optimisation was completed as before with both momenta set to zero. Optimisation was completed so that there was minimal oscillation (gradient of line =0) seen for the Internuclear Distance vs Time graph, as shown below. The optimised distances were found to be r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-F)=1.813 Å and r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-H)=0.7445 Å. &lt;br /&gt;
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[[File:Screenshot_2019-05-21_at_18.21.10.png|thumb|upright|400x400px|Graph showing Internuclear Distance vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
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===&#039;&#039;&#039;Q7 - Report the activation energy for both reactions.&#039;&#039;&#039;===&lt;br /&gt;
Below shows two graphs depicting the total energy plot of both reactions. The activation energy for both reactions can be calculated as the difference between the highest and lowest energy levels. &lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.37.01.png|500px|left|thumb|Graph of Energy vs Steps for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.41.09.png|500px|right|thumb|Graph of Energy vs Steps for HF + H.]]&lt;br /&gt;
|}&lt;br /&gt;
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&#039;&#039;&#039;Activation Energy(H + HF)&#039;&#039;&#039;= +31.22 kcalmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)&#039;&#039;&#039;= +0.130 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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{{fontcolor|pink|All correct and clearly presented with appropriate diagrams. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:01, 3 June 2019 (BST)}}&lt;br /&gt;
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===&#039;&#039;&#039;Q8 - 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.&#039;&#039;&#039;===&lt;br /&gt;
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For the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; a reactive trajectory was found using the following set of initial conditions: AB = 0.74 Å, BC = 1.80 Å, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5, and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.70. Using these intial conditions the graph of Momentum vs Time was produced, as seen below.&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.01.png|thumb|upright|400x400px|Graph of Momentum vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.11.png|thumb|upright|400x400px|Graph of Energy vs Time ]]&lt;br /&gt;
|}&lt;br /&gt;
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As you can see, whenever potential energy is lost, kinetic energy is gained by the same amount. Due to the exothermic nature of this reactrion, this kinetic energy is then converted into heat and can experimentally be seen by the increase in temperature.&lt;br /&gt;
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{{fontcolor|pink|Yes, that&#039;s right, can you think of a particular experimental setup/technique which can detect such a change in conditions accurately?[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:02, 3 June 2019 (BST)}}&lt;br /&gt;
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===&#039;&#039;&#039;Q9 - 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.&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s Rule states that vibrational energy is much less successful in promoting an early transition state than translational energy is. Additionally, the opposite is true - translational energy is more efficient in promoting a late transition state than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
As seen above when calculating the activation energy of reaction, the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Hammond&#039;s Postulate states that this reaction therefore has an early transition state. Using Polanyi&#039;s Rules, this reaction would be most effectively activated by translational energy. Similarly, for the reaction of H + HF (endothermic), this would be most efficiently activated by vibrational energy.&lt;br /&gt;
&lt;br /&gt;
For the first reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, I used the values of r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.74 Å, and r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=1.81 Å.  Then i looked at the contour plots for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-2.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-0.5 (Left diagram), and for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-2.5 (right diagram). For the initial set of conditions, there is greater vibrational energy, and the 2nd set of conditions, greater translational energy. &lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s Rules, we would expect this reaction to be best activated by vibrational energy. The two graphs below agree with these findings. &lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.32.46.png|thumb|upright|330x330px|Contour plot for greater vibrational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.33.04.png|thumb|upright|330x330px|Contour plot for greater translational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
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{{fontcolor|pink|I don&#039;t know whether I am just not managing to clearly decipher your figure, but the left diagram doesn&#039;t look reactive to me and the right one does. You haven&#039;t done any calculations wrong but you&#039;ve mixed up your order of Polanyi&#039;s rules. In an early barrier reaction, kinetic energy is effective in overcoming the barrier but vibrational energy is ineffective in overcoming the barrier. The distinction between the two systems would be clearer if you had one with high vibrational energy and low kinetic and vice versa. These both look like they have quite high vibrational energy. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:10, 3 June 2019 (BST)}}&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794075</id>
		<title>013366322</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794075"/>
		<updated>2019-06-03T12:02:33Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Q8 - 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;== EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system  ==&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q1 - 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?&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
On the potential energy surface, the transition state is the position along the minimum energy pathway, linking reactants and products, where potential is highest. The transition structure exists at a saddle point of the potential energy surface - that is when ∂V(&#039;&#039;&#039;ri&#039;&#039;&#039;)/∂(&#039;&#039;&#039;ri&#039;&#039;&#039;)=0. Furthermore, the 2nd partial derivatives with respect to the orthogonal vectors r1 and r2 have opposite signs; one is positive and the other negative. This tells us that this is a saddle point.&lt;br /&gt;
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[[File:Screenshot_2019-05-21_at_14.27.22.png|400px]]&lt;br /&gt;
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{{fontcolor|pink|Be careful to makesure you say &amp;quot;potential energy&amp;quot; not just &amp;quot;potential&amp;quot;. And yes this is all correct and clearly explained but you are missing part of the definition. The TS is a saddle point because it is the maximum along the reaction trajectory and a minimum in the orthogonal direction, so which vector r1 or r2 will be positive or negative? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:47, 3 June 2019 (BST)}}&lt;br /&gt;
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====&#039;&#039;&#039;Q2 - 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.&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 14.41.20.png|thumb|upright|400x400px|A graph showing Intermolecular distance Vs Time ]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_16.25.22.png|thumb|upright|400x400px|Contour Plot to find rts]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Firstly, we set AB=BC and momentum equal to 0. Then, plotting a graph of Internuclear Distance vs Time, we can find the transition state. The optimised distance is the distance at which there is no trajectory towards either reactants or products and at which oscillations are reduced producing a straight line as seen in the plot above. As the graph shows straight lines, we know there is no vibration, and the atoms stop moving. That is, potential energy is maximum and kinetic energy zero. As such, the optimised distance is found to be 0.9079 Å. Looking at the contour plot above, the transition state can also be seen in approximately the correct location, backing up the result.&lt;br /&gt;
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{{fontcolor|pink|Great explanation - very clear and well understood.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:50, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q3 - Comment on how the MEP and the trajectory you just calculated differ.&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_15.06.08.png|thumb|upright|400x400px|MEP Calculation]]&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 15.07.56.png|thumb|upright|400x400px|Dynamics Calculation]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The MEP graph shows no molecular vibration (as velocity=0) with momentum being equal to 0 in every time step. In comparison, the dynamics plot shows the vibrational energy of the molecule as seen by the non-straight line.&lt;br /&gt;
&lt;br /&gt;
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{{fontcolor|pink|True, can you think of why? In terms of the calculation process itself? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:54, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q4 - 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?&#039;&#039;&#039;===&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; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the trajectory !! Description of the dynamics &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || YES || [[File:Screenshot_dex_1.png|400x400px]] || Both reactants collide and have sufficient energy to surpass the activation barrier. Products are formed. Vibrational motion is also seen evident by the oscillations.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0  || -100.456 || NO || [[File:Screenshot_dex_2.png|400x400px]] || Atom C collides molecule AB but has insufficient kinetic energy to overcome the activation energy, thus not forming products. Molecules do not pass through the transition state.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5  || -98.956 || YES || [[File:Screenshot_dex_3.png|400x400px]] || Both molecules have sufficient energy to surpass the activation energy and so pass though the transition state, forming the products.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0  || -84.956 || NO || [[File:Screenshot_dex_4.png|400x400px]] || Both molecules have large energies and are able to overcome the activation energy. However, their energy is so great, that they recross the barrier and reform reactants.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2  || -83.416 || YES || [[File:Screenshot_dex_5.png|400x400px]] || Both molecules have sufficient energy to overcome the activation energy barrier, but have the potential to cross back over the barrier, and reform products. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It can be concluded that if reactants do not have sufficient kinetic energy to surpass the activation barrier, then the reaction will not occur. Furthermore, if the reactants have an excess of kinetic energy, the reaction also may not proceed as the products formed turn back into reactants.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Yes, or you could also say that there is not a simple threshold energy to determine whether or not the system will be reactive. It is not as simple as molecules that do have the activation energy will react, and molecules that don&#039;t won&#039;t react. That would be the simplest form of conclusion to be drawn from this. Your observations are clear and insightful. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:59, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q5 - State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Electron and nuclear motion are independent&lt;br /&gt;
Energy of the particles follows the Boltzmann distribution&lt;br /&gt;
Once reactants begin to combine and form the transition state, the transition state structure does not collapse to form reactants again&lt;br /&gt;
&lt;br /&gt;
Theory states that transition state structure does not collapse to reform the reactants. However, as experimental procedure shows, this can occur. As theory assumes that all reactions with sufficient energy will go onto form products, the real rate of reaction is much slower than in theory as reactants can be reformed.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Great![[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:00, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== EXERCISE 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q6 - 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?&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
 {|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_dex_f_h2.png|thumb|upright|400x400px|Surface Plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_dex_h_hf.png|thumb|upright|400x400px|Surface Plot for H + HF]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
As seen above, the surface plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; starts at a high energy position dropping down lower energy after the transition state. Therefore, this is an exothermic reaction. In contrast, for the surface plot of HF + H, the reaction starts at a low energy position and needs a large amount of energy to over come the activation energy barrier. After passing the transition state, the energy falls a small amount. This reaction is therefore endothermic. From this, we can conclude that the HF bond is stronger than the HH bond since HF is lower in energy than HH. &lt;br /&gt;
&lt;br /&gt;
Furthermore, Hammond&#039;s Postulate states that the transition state will resemble either the product or reactants, whichever it is closer to in energy. To find the transition state, optimisation was completed as before with both momenta set to zero. Optimisation was completed so that there was minimal oscillation (gradient of line =0) seen for the Internuclear Distance vs Time graph, as shown below. The optimised distances were found to be r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-F)=1.813 Å and r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-H)=0.7445 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:Screenshot_2019-05-21_at_18.21.10.png|thumb|upright|400x400px|Graph showing Internuclear Distance vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
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===&#039;&#039;&#039;Q7 - Report the activation energy for both reactions.&#039;&#039;&#039;===&lt;br /&gt;
Below shows two graphs depicting the total energy plot of both reactions. The activation energy for both reactions can be calculated as the difference between the highest and lowest energy levels. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.37.01.png|500px|left|thumb|Graph of Energy vs Steps for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.41.09.png|500px|right|thumb|Graph of Energy vs Steps for HF + H.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(H + HF)&#039;&#039;&#039;= +31.22 kcalmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)&#039;&#039;&#039;= +0.130 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|All correct and clearly presented with appropriate diagrams. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:01, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q8 - 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.&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; a reactive trajectory was found using the following set of initial conditions: AB = 0.74 Å, BC = 1.80 Å, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5, and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.70. Using these intial conditions the graph of Momentum vs Time was produced, as seen below.&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.01.png|thumb|upright|400x400px|Graph of Momentum vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.11.png|thumb|upright|400x400px|Graph of Energy vs Time ]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
As you can see, whenever potential energy is lost, kinetic energy is gained by the same amount. Due to the exothermic nature of this reactrion, this kinetic energy is then converted into heat and can experimentally be seen by the increase in temperature.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Yes, that&#039;s right, can you think of a particular experimental setup/technique which can detect such a change in conditions accurately?[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:02, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q9 - 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.&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s Rule states that vibrational energy is much less successful in promoting an early transition state than translational energy is. Additionally, the opposite is true - translational energy is more efficient in promoting a late transition state than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
As seen above when calculating the activation energy of reaction, the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Hammond&#039;s Postulate states that this reaction therefore has an early transition state. Using Polanyi&#039;s Rules, this reaction would be most effectively activated by translational energy. Similarly, for the reaction of H + HF (endothermic), this would be most efficiently activated by vibrational energy.&lt;br /&gt;
&lt;br /&gt;
For the first reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, I used the values of r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.74 Å, and r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=1.81 Å.  Then i looked at the contour plots for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-2.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-0.5 (Left diagram), and for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-2.5 (right diagram). For the initial set of conditions, there is greater vibrational energy, and the 2nd set of conditions, greater translational energy. &lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s Rules, we would expect this reaction to be best activated by vibrational energy. The two graphs below agree with these findings. &lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.32.46.png|thumb|upright|330x330px|Contour plot for greater vibrational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.33.04.png|thumb|upright|330x330px|Contour plot for greater translational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794073</id>
		<title>013366322</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794073"/>
		<updated>2019-06-03T12:01:44Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Q7 - Report the activation energy for both reactions. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system  ==&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q1 - 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?&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
On the potential energy surface, the transition state is the position along the minimum energy pathway, linking reactants and products, where potential is highest. The transition structure exists at a saddle point of the potential energy surface - that is when ∂V(&#039;&#039;&#039;ri&#039;&#039;&#039;)/∂(&#039;&#039;&#039;ri&#039;&#039;&#039;)=0. Furthermore, the 2nd partial derivatives with respect to the orthogonal vectors r1 and r2 have opposite signs; one is positive and the other negative. This tells us that this is a saddle point.&lt;br /&gt;
&lt;br /&gt;
[[File:Screenshot_2019-05-21_at_14.27.22.png|400px]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Be careful to makesure you say &amp;quot;potential energy&amp;quot; not just &amp;quot;potential&amp;quot;. And yes this is all correct and clearly explained but you are missing part of the definition. The TS is a saddle point because it is the maximum along the reaction trajectory and a minimum in the orthogonal direction, so which vector r1 or r2 will be positive or negative? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:47, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q2 - 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.&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 14.41.20.png|thumb|upright|400x400px|A graph showing Intermolecular distance Vs Time ]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_16.25.22.png|thumb|upright|400x400px|Contour Plot to find rts]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Firstly, we set AB=BC and momentum equal to 0. Then, plotting a graph of Internuclear Distance vs Time, we can find the transition state. The optimised distance is the distance at which there is no trajectory towards either reactants or products and at which oscillations are reduced producing a straight line as seen in the plot above. As the graph shows straight lines, we know there is no vibration, and the atoms stop moving. That is, potential energy is maximum and kinetic energy zero. As such, the optimised distance is found to be 0.9079 Å. Looking at the contour plot above, the transition state can also be seen in approximately the correct location, backing up the result.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Great explanation - very clear and well understood.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:50, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q3 - Comment on how the MEP and the trajectory you just calculated differ.&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_15.06.08.png|thumb|upright|400x400px|MEP Calculation]]&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 15.07.56.png|thumb|upright|400x400px|Dynamics Calculation]]&lt;br /&gt;
|}&lt;br /&gt;
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The MEP graph shows no molecular vibration (as velocity=0) with momentum being equal to 0 in every time step. In comparison, the dynamics plot shows the vibrational energy of the molecule as seen by the non-straight line.&lt;br /&gt;
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{{fontcolor|pink|True, can you think of why? In terms of the calculation process itself? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:54, 3 June 2019 (BST)}}&lt;br /&gt;
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===&#039;&#039;&#039;Q4 - 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?&#039;&#039;&#039;===&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; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the trajectory !! Description of the dynamics &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || YES || [[File:Screenshot_dex_1.png|400x400px]] || Both reactants collide and have sufficient energy to surpass the activation barrier. Products are formed. Vibrational motion is also seen evident by the oscillations.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0  || -100.456 || NO || [[File:Screenshot_dex_2.png|400x400px]] || Atom C collides molecule AB but has insufficient kinetic energy to overcome the activation energy, thus not forming products. Molecules do not pass through the transition state.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5  || -98.956 || YES || [[File:Screenshot_dex_3.png|400x400px]] || Both molecules have sufficient energy to surpass the activation energy and so pass though the transition state, forming the products.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0  || -84.956 || NO || [[File:Screenshot_dex_4.png|400x400px]] || Both molecules have large energies and are able to overcome the activation energy. However, their energy is so great, that they recross the barrier and reform reactants.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2  || -83.416 || YES || [[File:Screenshot_dex_5.png|400x400px]] || Both molecules have sufficient energy to overcome the activation energy barrier, but have the potential to cross back over the barrier, and reform products. &lt;br /&gt;
|}&lt;br /&gt;
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It can be concluded that if reactants do not have sufficient kinetic energy to surpass the activation barrier, then the reaction will not occur. Furthermore, if the reactants have an excess of kinetic energy, the reaction also may not proceed as the products formed turn back into reactants.&lt;br /&gt;
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{{fontcolor|pink|Yes, or you could also say that there is not a simple threshold energy to determine whether or not the system will be reactive. It is not as simple as molecules that do have the activation energy will react, and molecules that don&#039;t won&#039;t react. That would be the simplest form of conclusion to be drawn from this. Your observations are clear and insightful. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:59, 3 June 2019 (BST)}}&lt;br /&gt;
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===&#039;&#039;&#039;Q5 - State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Electron and nuclear motion are independent&lt;br /&gt;
Energy of the particles follows the Boltzmann distribution&lt;br /&gt;
Once reactants begin to combine and form the transition state, the transition state structure does not collapse to form reactants again&lt;br /&gt;
&lt;br /&gt;
Theory states that transition state structure does not collapse to reform the reactants. However, as experimental procedure shows, this can occur. As theory assumes that all reactions with sufficient energy will go onto form products, the real rate of reaction is much slower than in theory as reactants can be reformed.&lt;br /&gt;
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{{fontcolor|pink| Great![[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:00, 3 June 2019 (BST)}}&lt;br /&gt;
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== EXERCISE 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q6 - 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?&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
 {|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_dex_f_h2.png|thumb|upright|400x400px|Surface Plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_dex_h_hf.png|thumb|upright|400x400px|Surface Plot for H + HF]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
As seen above, the surface plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; starts at a high energy position dropping down lower energy after the transition state. Therefore, this is an exothermic reaction. In contrast, for the surface plot of HF + H, the reaction starts at a low energy position and needs a large amount of energy to over come the activation energy barrier. After passing the transition state, the energy falls a small amount. This reaction is therefore endothermic. From this, we can conclude that the HF bond is stronger than the HH bond since HF is lower in energy than HH. &lt;br /&gt;
&lt;br /&gt;
Furthermore, Hammond&#039;s Postulate states that the transition state will resemble either the product or reactants, whichever it is closer to in energy. To find the transition state, optimisation was completed as before with both momenta set to zero. Optimisation was completed so that there was minimal oscillation (gradient of line =0) seen for the Internuclear Distance vs Time graph, as shown below. The optimised distances were found to be r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-F)=1.813 Å and r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-H)=0.7445 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:Screenshot_2019-05-21_at_18.21.10.png|thumb|upright|400x400px|Graph showing Internuclear Distance vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
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===&#039;&#039;&#039;Q7 - Report the activation energy for both reactions.&#039;&#039;&#039;===&lt;br /&gt;
Below shows two graphs depicting the total energy plot of both reactions. The activation energy for both reactions can be calculated as the difference between the highest and lowest energy levels. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.37.01.png|500px|left|thumb|Graph of Energy vs Steps for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.41.09.png|500px|right|thumb|Graph of Energy vs Steps for HF + H.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(H + HF)&#039;&#039;&#039;= +31.22 kcalmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)&#039;&#039;&#039;= +0.130 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|All correct and clearly presented with appropriate diagrams. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:01, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q8 - 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.&#039;&#039;&#039;===&lt;br /&gt;
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For the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; a reactive trajectory was found using the following set of initial conditions: AB = 0.74 Å, BC = 1.80 Å, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5, and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.70. Using these intial conditions the graph of Momentum vs Time was produced, as seen below.&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.01.png|thumb|upright|400x400px|Graph of Momentum vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.11.png|thumb|upright|400x400px|Graph of Energy vs Time ]]&lt;br /&gt;
|}&lt;br /&gt;
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As you can see, whenever potential energy is lost, kinetic energy is gained by the same amount. Due to the exothermic nature of this reactrion, this kinetic energy is then converted into heat and can experimentally be seen by the increase in temperature.&lt;br /&gt;
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===&#039;&#039;&#039;Q9 - 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.&#039;&#039;&#039;===&lt;br /&gt;
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Polanyi&#039;s Rule states that vibrational energy is much less successful in promoting an early transition state than translational energy is. Additionally, the opposite is true - translational energy is more efficient in promoting a late transition state than vibrational energy.&lt;br /&gt;
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As seen above when calculating the activation energy of reaction, the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Hammond&#039;s Postulate states that this reaction therefore has an early transition state. Using Polanyi&#039;s Rules, this reaction would be most effectively activated by translational energy. Similarly, for the reaction of H + HF (endothermic), this would be most efficiently activated by vibrational energy.&lt;br /&gt;
&lt;br /&gt;
For the first reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, I used the values of r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.74 Å, and r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=1.81 Å.  Then i looked at the contour plots for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-2.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-0.5 (Left diagram), and for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-2.5 (right diagram). For the initial set of conditions, there is greater vibrational energy, and the 2nd set of conditions, greater translational energy. &lt;br /&gt;
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According to Polanyi&#039;s Rules, we would expect this reaction to be best activated by vibrational energy. The two graphs below agree with these findings. &lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.32.46.png|thumb|upright|330x330px|Contour plot for greater vibrational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.33.04.png|thumb|upright|330x330px|Contour plot for greater translational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794072</id>
		<title>013366322</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794072"/>
		<updated>2019-06-03T12:00:23Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Q5 - State what are the main assumptions of Transition State Theory. 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;== EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system  ==&lt;br /&gt;
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====&#039;&#039;&#039;Q1 - 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?&#039;&#039;&#039;====&lt;br /&gt;
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On the potential energy surface, the transition state is the position along the minimum energy pathway, linking reactants and products, where potential is highest. The transition structure exists at a saddle point of the potential energy surface - that is when ∂V(&#039;&#039;&#039;ri&#039;&#039;&#039;)/∂(&#039;&#039;&#039;ri&#039;&#039;&#039;)=0. Furthermore, the 2nd partial derivatives with respect to the orthogonal vectors r1 and r2 have opposite signs; one is positive and the other negative. This tells us that this is a saddle point.&lt;br /&gt;
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[[File:Screenshot_2019-05-21_at_14.27.22.png|400px]]&lt;br /&gt;
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{{fontcolor|pink|Be careful to makesure you say &amp;quot;potential energy&amp;quot; not just &amp;quot;potential&amp;quot;. And yes this is all correct and clearly explained but you are missing part of the definition. The TS is a saddle point because it is the maximum along the reaction trajectory and a minimum in the orthogonal direction, so which vector r1 or r2 will be positive or negative? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:47, 3 June 2019 (BST)}}&lt;br /&gt;
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====&#039;&#039;&#039;Q2 - 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.&#039;&#039;&#039;====&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 14.41.20.png|thumb|upright|400x400px|A graph showing Intermolecular distance Vs Time ]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_16.25.22.png|thumb|upright|400x400px|Contour Plot to find rts]]&lt;br /&gt;
|}&lt;br /&gt;
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Firstly, we set AB=BC and momentum equal to 0. Then, plotting a graph of Internuclear Distance vs Time, we can find the transition state. The optimised distance is the distance at which there is no trajectory towards either reactants or products and at which oscillations are reduced producing a straight line as seen in the plot above. As the graph shows straight lines, we know there is no vibration, and the atoms stop moving. That is, potential energy is maximum and kinetic energy zero. As such, the optimised distance is found to be 0.9079 Å. Looking at the contour plot above, the transition state can also be seen in approximately the correct location, backing up the result.&lt;br /&gt;
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{{fontcolor|pink|Great explanation - very clear and well understood.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:50, 3 June 2019 (BST)}}&lt;br /&gt;
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====&#039;&#039;&#039;Q3 - Comment on how the MEP and the trajectory you just calculated differ.&#039;&#039;&#039;====&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_15.06.08.png|thumb|upright|400x400px|MEP Calculation]]&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 15.07.56.png|thumb|upright|400x400px|Dynamics Calculation]]&lt;br /&gt;
|}&lt;br /&gt;
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The MEP graph shows no molecular vibration (as velocity=0) with momentum being equal to 0 in every time step. In comparison, the dynamics plot shows the vibrational energy of the molecule as seen by the non-straight line.&lt;br /&gt;
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{{fontcolor|pink|True, can you think of why? In terms of the calculation process itself? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:54, 3 June 2019 (BST)}}&lt;br /&gt;
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===&#039;&#039;&#039;Q4 - 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?&#039;&#039;&#039;===&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; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the trajectory !! Description of the dynamics &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || YES || [[File:Screenshot_dex_1.png|400x400px]] || Both reactants collide and have sufficient energy to surpass the activation barrier. Products are formed. Vibrational motion is also seen evident by the oscillations.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0  || -100.456 || NO || [[File:Screenshot_dex_2.png|400x400px]] || Atom C collides molecule AB but has insufficient kinetic energy to overcome the activation energy, thus not forming products. Molecules do not pass through the transition state.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5  || -98.956 || YES || [[File:Screenshot_dex_3.png|400x400px]] || Both molecules have sufficient energy to surpass the activation energy and so pass though the transition state, forming the products.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0  || -84.956 || NO || [[File:Screenshot_dex_4.png|400x400px]] || Both molecules have large energies and are able to overcome the activation energy. However, their energy is so great, that they recross the barrier and reform reactants.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2  || -83.416 || YES || [[File:Screenshot_dex_5.png|400x400px]] || Both molecules have sufficient energy to overcome the activation energy barrier, but have the potential to cross back over the barrier, and reform products. &lt;br /&gt;
|}&lt;br /&gt;
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It can be concluded that if reactants do not have sufficient kinetic energy to surpass the activation barrier, then the reaction will not occur. Furthermore, if the reactants have an excess of kinetic energy, the reaction also may not proceed as the products formed turn back into reactants.&lt;br /&gt;
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{{fontcolor|pink|Yes, or you could also say that there is not a simple threshold energy to determine whether or not the system will be reactive. It is not as simple as molecules that do have the activation energy will react, and molecules that don&#039;t won&#039;t react. That would be the simplest form of conclusion to be drawn from this. Your observations are clear and insightful. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:59, 3 June 2019 (BST)}}&lt;br /&gt;
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===&#039;&#039;&#039;Q5 - State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;===&lt;br /&gt;
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Electron and nuclear motion are independent&lt;br /&gt;
Energy of the particles follows the Boltzmann distribution&lt;br /&gt;
Once reactants begin to combine and form the transition state, the transition state structure does not collapse to form reactants again&lt;br /&gt;
&lt;br /&gt;
Theory states that transition state structure does not collapse to reform the reactants. However, as experimental procedure shows, this can occur. As theory assumes that all reactions with sufficient energy will go onto form products, the real rate of reaction is much slower than in theory as reactants can be reformed.&lt;br /&gt;
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{{fontcolor|pink| Great![[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 13:00, 3 June 2019 (BST)}}&lt;br /&gt;
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== EXERCISE 2: F - H - H system ==&lt;br /&gt;
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===&#039;&#039;&#039;Q6 - 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?&#039;&#039;&#039;===&lt;br /&gt;
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 {|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_dex_f_h2.png|thumb|upright|400x400px|Surface Plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_dex_h_hf.png|thumb|upright|400x400px|Surface Plot for H + HF]]&lt;br /&gt;
|}&lt;br /&gt;
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As seen above, the surface plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; starts at a high energy position dropping down lower energy after the transition state. Therefore, this is an exothermic reaction. In contrast, for the surface plot of HF + H, the reaction starts at a low energy position and needs a large amount of energy to over come the activation energy barrier. After passing the transition state, the energy falls a small amount. This reaction is therefore endothermic. From this, we can conclude that the HF bond is stronger than the HH bond since HF is lower in energy than HH. &lt;br /&gt;
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Furthermore, Hammond&#039;s Postulate states that the transition state will resemble either the product or reactants, whichever it is closer to in energy. To find the transition state, optimisation was completed as before with both momenta set to zero. Optimisation was completed so that there was minimal oscillation (gradient of line =0) seen for the Internuclear Distance vs Time graph, as shown below. The optimised distances were found to be r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-F)=1.813 Å and r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-H)=0.7445 Å. &lt;br /&gt;
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[[File:Screenshot_2019-05-21_at_18.21.10.png|thumb|upright|400x400px|Graph showing Internuclear Distance vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
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===&#039;&#039;&#039;Q7 - Report the activation energy for both reactions.&#039;&#039;&#039;===&lt;br /&gt;
Below shows two graphs depicting the total energy plot of both reactions. The activation energy for both reactions can be calculated as the difference between the highest and lowest energy levels. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.37.01.png|500px|left|thumb|Graph of Energy vs Steps for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.41.09.png|500px|right|thumb|Graph of Energy vs Steps for HF + H.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(H + HF)&#039;&#039;&#039;= +31.22 kcalmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)&#039;&#039;&#039;= +0.130 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q8 - 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.&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; a reactive trajectory was found using the following set of initial conditions: AB = 0.74 Å, BC = 1.80 Å, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5, and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.70. Using these intial conditions the graph of Momentum vs Time was produced, as seen below.&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.01.png|thumb|upright|400x400px|Graph of Momentum vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.11.png|thumb|upright|400x400px|Graph of Energy vs Time ]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
As you can see, whenever potential energy is lost, kinetic energy is gained by the same amount. Due to the exothermic nature of this reactrion, this kinetic energy is then converted into heat and can experimentally be seen by the increase in temperature.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q9 - 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.&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s Rule states that vibrational energy is much less successful in promoting an early transition state than translational energy is. Additionally, the opposite is true - translational energy is more efficient in promoting a late transition state than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
As seen above when calculating the activation energy of reaction, the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Hammond&#039;s Postulate states that this reaction therefore has an early transition state. Using Polanyi&#039;s Rules, this reaction would be most effectively activated by translational energy. Similarly, for the reaction of H + HF (endothermic), this would be most efficiently activated by vibrational energy.&lt;br /&gt;
&lt;br /&gt;
For the first reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, I used the values of r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.74 Å, and r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=1.81 Å.  Then i looked at the contour plots for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-2.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-0.5 (Left diagram), and for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-2.5 (right diagram). For the initial set of conditions, there is greater vibrational energy, and the 2nd set of conditions, greater translational energy. &lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s Rules, we would expect this reaction to be best activated by vibrational energy. The two graphs below agree with these findings. &lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.32.46.png|thumb|upright|330x330px|Contour plot for greater vibrational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.33.04.png|thumb|upright|330x330px|Contour plot for greater translational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794071</id>
		<title>013366322</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794071"/>
		<updated>2019-06-03T11:59:50Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Q4 - 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&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system  ==&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q1 - 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?&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
On the potential energy surface, the transition state is the position along the minimum energy pathway, linking reactants and products, where potential is highest. The transition structure exists at a saddle point of the potential energy surface - that is when ∂V(&#039;&#039;&#039;ri&#039;&#039;&#039;)/∂(&#039;&#039;&#039;ri&#039;&#039;&#039;)=0. Furthermore, the 2nd partial derivatives with respect to the orthogonal vectors r1 and r2 have opposite signs; one is positive and the other negative. This tells us that this is a saddle point.&lt;br /&gt;
&lt;br /&gt;
[[File:Screenshot_2019-05-21_at_14.27.22.png|400px]]&lt;br /&gt;
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{{fontcolor|pink|Be careful to makesure you say &amp;quot;potential energy&amp;quot; not just &amp;quot;potential&amp;quot;. And yes this is all correct and clearly explained but you are missing part of the definition. The TS is a saddle point because it is the maximum along the reaction trajectory and a minimum in the orthogonal direction, so which vector r1 or r2 will be positive or negative? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:47, 3 June 2019 (BST)}}&lt;br /&gt;
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====&#039;&#039;&#039;Q2 - 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.&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 14.41.20.png|thumb|upright|400x400px|A graph showing Intermolecular distance Vs Time ]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_16.25.22.png|thumb|upright|400x400px|Contour Plot to find rts]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Firstly, we set AB=BC and momentum equal to 0. Then, plotting a graph of Internuclear Distance vs Time, we can find the transition state. The optimised distance is the distance at which there is no trajectory towards either reactants or products and at which oscillations are reduced producing a straight line as seen in the plot above. As the graph shows straight lines, we know there is no vibration, and the atoms stop moving. That is, potential energy is maximum and kinetic energy zero. As such, the optimised distance is found to be 0.9079 Å. Looking at the contour plot above, the transition state can also be seen in approximately the correct location, backing up the result.&lt;br /&gt;
&lt;br /&gt;
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{{fontcolor|pink|Great explanation - very clear and well understood.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:50, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q3 - Comment on how the MEP and the trajectory you just calculated differ.&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_15.06.08.png|thumb|upright|400x400px|MEP Calculation]]&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 15.07.56.png|thumb|upright|400x400px|Dynamics Calculation]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The MEP graph shows no molecular vibration (as velocity=0) with momentum being equal to 0 in every time step. In comparison, the dynamics plot shows the vibrational energy of the molecule as seen by the non-straight line.&lt;br /&gt;
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{{fontcolor|pink|True, can you think of why? In terms of the calculation process itself? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:54, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q4 - 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?&#039;&#039;&#039;===&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; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the trajectory !! Description of the dynamics &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || YES || [[File:Screenshot_dex_1.png|400x400px]] || Both reactants collide and have sufficient energy to surpass the activation barrier. Products are formed. Vibrational motion is also seen evident by the oscillations.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0  || -100.456 || NO || [[File:Screenshot_dex_2.png|400x400px]] || Atom C collides molecule AB but has insufficient kinetic energy to overcome the activation energy, thus not forming products. Molecules do not pass through the transition state.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5  || -98.956 || YES || [[File:Screenshot_dex_3.png|400x400px]] || Both molecules have sufficient energy to surpass the activation energy and so pass though the transition state, forming the products.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0  || -84.956 || NO || [[File:Screenshot_dex_4.png|400x400px]] || Both molecules have large energies and are able to overcome the activation energy. However, their energy is so great, that they recross the barrier and reform reactants.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2  || -83.416 || YES || [[File:Screenshot_dex_5.png|400x400px]] || Both molecules have sufficient energy to overcome the activation energy barrier, but have the potential to cross back over the barrier, and reform products. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It can be concluded that if reactants do not have sufficient kinetic energy to surpass the activation barrier, then the reaction will not occur. Furthermore, if the reactants have an excess of kinetic energy, the reaction also may not proceed as the products formed turn back into reactants.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Yes, or you could also say that there is not a simple threshold energy to determine whether or not the system will be reactive. It is not as simple as molecules that do have the activation energy will react, and molecules that don&#039;t won&#039;t react. That would be the simplest form of conclusion to be drawn from this. Your observations are clear and insightful. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:59, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q5 - State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Electron and nuclear motion are independent&lt;br /&gt;
Energy of the particles follows the Boltzmann distribution&lt;br /&gt;
Once reactants begin to combine and form the transition state, the transition state structure does not collapse to form reactants again&lt;br /&gt;
&lt;br /&gt;
Theory states that transition state structure does not collapse to reform the reactants. However, as experimental procedure shows, this can occur. As theory assumes that all reactions with sufficient energy will go onto form products, the real rate of reaction is much slower than in theory as reactants can be reformed. &lt;br /&gt;
&lt;br /&gt;
== EXERCISE 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q6 - 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?&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
 {|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_dex_f_h2.png|thumb|upright|400x400px|Surface Plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_dex_h_hf.png|thumb|upright|400x400px|Surface Plot for H + HF]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
As seen above, the surface plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; starts at a high energy position dropping down lower energy after the transition state. Therefore, this is an exothermic reaction. In contrast, for the surface plot of HF + H, the reaction starts at a low energy position and needs a large amount of energy to over come the activation energy barrier. After passing the transition state, the energy falls a small amount. This reaction is therefore endothermic. From this, we can conclude that the HF bond is stronger than the HH bond since HF is lower in energy than HH. &lt;br /&gt;
&lt;br /&gt;
Furthermore, Hammond&#039;s Postulate states that the transition state will resemble either the product or reactants, whichever it is closer to in energy. To find the transition state, optimisation was completed as before with both momenta set to zero. Optimisation was completed so that there was minimal oscillation (gradient of line =0) seen for the Internuclear Distance vs Time graph, as shown below. The optimised distances were found to be r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-F)=1.813 Å and r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-H)=0.7445 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:Screenshot_2019-05-21_at_18.21.10.png|thumb|upright|400x400px|Graph showing Internuclear Distance vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
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===&#039;&#039;&#039;Q7 - Report the activation energy for both reactions.&#039;&#039;&#039;===&lt;br /&gt;
Below shows two graphs depicting the total energy plot of both reactions. The activation energy for both reactions can be calculated as the difference between the highest and lowest energy levels. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.37.01.png|500px|left|thumb|Graph of Energy vs Steps for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.41.09.png|500px|right|thumb|Graph of Energy vs Steps for HF + H.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(H + HF)&#039;&#039;&#039;= +31.22 kcalmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)&#039;&#039;&#039;= +0.130 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q8 - 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.&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; a reactive trajectory was found using the following set of initial conditions: AB = 0.74 Å, BC = 1.80 Å, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5, and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.70. Using these intial conditions the graph of Momentum vs Time was produced, as seen below.&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.01.png|thumb|upright|400x400px|Graph of Momentum vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.11.png|thumb|upright|400x400px|Graph of Energy vs Time ]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
As you can see, whenever potential energy is lost, kinetic energy is gained by the same amount. Due to the exothermic nature of this reactrion, this kinetic energy is then converted into heat and can experimentally be seen by the increase in temperature.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q9 - 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.&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s Rule states that vibrational energy is much less successful in promoting an early transition state than translational energy is. Additionally, the opposite is true - translational energy is more efficient in promoting a late transition state than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
As seen above when calculating the activation energy of reaction, the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Hammond&#039;s Postulate states that this reaction therefore has an early transition state. Using Polanyi&#039;s Rules, this reaction would be most effectively activated by translational energy. Similarly, for the reaction of H + HF (endothermic), this would be most efficiently activated by vibrational energy.&lt;br /&gt;
&lt;br /&gt;
For the first reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, I used the values of r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.74 Å, and r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=1.81 Å.  Then i looked at the contour plots for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-2.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-0.5 (Left diagram), and for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-2.5 (right diagram). For the initial set of conditions, there is greater vibrational energy, and the 2nd set of conditions, greater translational energy. &lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s Rules, we would expect this reaction to be best activated by vibrational energy. The two graphs below agree with these findings. &lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.32.46.png|thumb|upright|330x330px|Contour plot for greater vibrational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.33.04.png|thumb|upright|330x330px|Contour plot for greater translational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794070</id>
		<title>013366322</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794070"/>
		<updated>2019-06-03T11:54:56Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Q3 - 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&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system  ==&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q1 - 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?&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
On the potential energy surface, the transition state is the position along the minimum energy pathway, linking reactants and products, where potential is highest. The transition structure exists at a saddle point of the potential energy surface - that is when ∂V(&#039;&#039;&#039;ri&#039;&#039;&#039;)/∂(&#039;&#039;&#039;ri&#039;&#039;&#039;)=0. Furthermore, the 2nd partial derivatives with respect to the orthogonal vectors r1 and r2 have opposite signs; one is positive and the other negative. This tells us that this is a saddle point.&lt;br /&gt;
&lt;br /&gt;
[[File:Screenshot_2019-05-21_at_14.27.22.png|400px]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Be careful to makesure you say &amp;quot;potential energy&amp;quot; not just &amp;quot;potential&amp;quot;. And yes this is all correct and clearly explained but you are missing part of the definition. The TS is a saddle point because it is the maximum along the reaction trajectory and a minimum in the orthogonal direction, so which vector r1 or r2 will be positive or negative? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:47, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q2 - 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.&#039;&#039;&#039;====&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 14.41.20.png|thumb|upright|400x400px|A graph showing Intermolecular distance Vs Time ]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_16.25.22.png|thumb|upright|400x400px|Contour Plot to find rts]]&lt;br /&gt;
|}&lt;br /&gt;
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Firstly, we set AB=BC and momentum equal to 0. Then, plotting a graph of Internuclear Distance vs Time, we can find the transition state. The optimised distance is the distance at which there is no trajectory towards either reactants or products and at which oscillations are reduced producing a straight line as seen in the plot above. As the graph shows straight lines, we know there is no vibration, and the atoms stop moving. That is, potential energy is maximum and kinetic energy zero. As such, the optimised distance is found to be 0.9079 Å. Looking at the contour plot above, the transition state can also be seen in approximately the correct location, backing up the result.&lt;br /&gt;
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{{fontcolor|pink|Great explanation - very clear and well understood.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:50, 3 June 2019 (BST)}}&lt;br /&gt;
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====&#039;&#039;&#039;Q3 - Comment on how the MEP and the trajectory you just calculated differ.&#039;&#039;&#039;====&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_15.06.08.png|thumb|upright|400x400px|MEP Calculation]]&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 15.07.56.png|thumb|upright|400x400px|Dynamics Calculation]]&lt;br /&gt;
|}&lt;br /&gt;
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The MEP graph shows no molecular vibration (as velocity=0) with momentum being equal to 0 in every time step. In comparison, the dynamics plot shows the vibrational energy of the molecule as seen by the non-straight line.&lt;br /&gt;
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{{fontcolor|pink|True, can you think of why? In terms of the calculation process itself? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:54, 3 June 2019 (BST)}}&lt;br /&gt;
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===&#039;&#039;&#039;Q4 - 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?&#039;&#039;&#039;===&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; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the trajectory !! Description of the dynamics &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || YES || [[File:Screenshot_dex_1.png|400x400px]] || Both reactants collide and have sufficient energy to surpass the activation barrier. Products are formed. Vibrational motion is also seen evident by the oscillations.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0  || -100.456 || NO || [[File:Screenshot_dex_2.png|400x400px]] || Atom C collides molecule AB but has insufficient kinetic energy to overcome the activation energy, thus not forming products. Molecules do not pass through the transition state.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5  || -98.956 || YES || [[File:Screenshot_dex_3.png|400x400px]] || Both molecules have sufficient energy to surpass the activation energy and so pass though the transition state, forming the products.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0  || -84.956 || NO || [[File:Screenshot_dex_4.png|400x400px]] || Both molecules have large energies and are able to overcome the activation energy. However, their energy is so great, that they recross the barrier and reform reactants.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2  || -83.416 || YES || [[File:Screenshot_dex_5.png|400x400px]] || Both molecules have sufficient energy to overcome the activation energy barrier, but have the potential to cross back over the barrier, and reform products. &lt;br /&gt;
|}&lt;br /&gt;
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It can be concluded that if reactants do not have sufficient kinetic energy to surpass the activation barrier, then the reaction will not occur. Furthermore, if the reactants have an excess of kinetic energy, the reaction also may not proceed as the products formed turn back into reactants.&lt;br /&gt;
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===&#039;&#039;&#039;Q5 - State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;===&lt;br /&gt;
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Electron and nuclear motion are independent&lt;br /&gt;
Energy of the particles follows the Boltzmann distribution&lt;br /&gt;
Once reactants begin to combine and form the transition state, the transition state structure does not collapse to form reactants again&lt;br /&gt;
&lt;br /&gt;
Theory states that transition state structure does not collapse to reform the reactants. However, as experimental procedure shows, this can occur. As theory assumes that all reactions with sufficient energy will go onto form products, the real rate of reaction is much slower than in theory as reactants can be reformed. &lt;br /&gt;
&lt;br /&gt;
== EXERCISE 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q6 - 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?&#039;&#039;&#039;===&lt;br /&gt;
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 {|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_dex_f_h2.png|thumb|upright|400x400px|Surface Plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_dex_h_hf.png|thumb|upright|400x400px|Surface Plot for H + HF]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
As seen above, the surface plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; starts at a high energy position dropping down lower energy after the transition state. Therefore, this is an exothermic reaction. In contrast, for the surface plot of HF + H, the reaction starts at a low energy position and needs a large amount of energy to over come the activation energy barrier. After passing the transition state, the energy falls a small amount. This reaction is therefore endothermic. From this, we can conclude that the HF bond is stronger than the HH bond since HF is lower in energy than HH. &lt;br /&gt;
&lt;br /&gt;
Furthermore, Hammond&#039;s Postulate states that the transition state will resemble either the product or reactants, whichever it is closer to in energy. To find the transition state, optimisation was completed as before with both momenta set to zero. Optimisation was completed so that there was minimal oscillation (gradient of line =0) seen for the Internuclear Distance vs Time graph, as shown below. The optimised distances were found to be r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-F)=1.813 Å and r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-H)=0.7445 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:Screenshot_2019-05-21_at_18.21.10.png|thumb|upright|400x400px|Graph showing Internuclear Distance vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
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===&#039;&#039;&#039;Q7 - Report the activation energy for both reactions.&#039;&#039;&#039;===&lt;br /&gt;
Below shows two graphs depicting the total energy plot of both reactions. The activation energy for both reactions can be calculated as the difference between the highest and lowest energy levels. &lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.37.01.png|500px|left|thumb|Graph of Energy vs Steps for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.41.09.png|500px|right|thumb|Graph of Energy vs Steps for HF + H.]]&lt;br /&gt;
|}&lt;br /&gt;
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&#039;&#039;&#039;Activation Energy(H + HF)&#039;&#039;&#039;= +31.22 kcalmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)&#039;&#039;&#039;= +0.130 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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===&#039;&#039;&#039;Q8 - 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.&#039;&#039;&#039;===&lt;br /&gt;
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For the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; a reactive trajectory was found using the following set of initial conditions: AB = 0.74 Å, BC = 1.80 Å, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5, and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.70. Using these intial conditions the graph of Momentum vs Time was produced, as seen below.&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.01.png|thumb|upright|400x400px|Graph of Momentum vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.11.png|thumb|upright|400x400px|Graph of Energy vs Time ]]&lt;br /&gt;
|}&lt;br /&gt;
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As you can see, whenever potential energy is lost, kinetic energy is gained by the same amount. Due to the exothermic nature of this reactrion, this kinetic energy is then converted into heat and can experimentally be seen by the increase in temperature.&lt;br /&gt;
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===&#039;&#039;&#039;Q9 - 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.&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s Rule states that vibrational energy is much less successful in promoting an early transition state than translational energy is. Additionally, the opposite is true - translational energy is more efficient in promoting a late transition state than vibrational energy.&lt;br /&gt;
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As seen above when calculating the activation energy of reaction, the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Hammond&#039;s Postulate states that this reaction therefore has an early transition state. Using Polanyi&#039;s Rules, this reaction would be most effectively activated by translational energy. Similarly, for the reaction of H + HF (endothermic), this would be most efficiently activated by vibrational energy.&lt;br /&gt;
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For the first reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, I used the values of r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.74 Å, and r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=1.81 Å.  Then i looked at the contour plots for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-2.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-0.5 (Left diagram), and for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-2.5 (right diagram). For the initial set of conditions, there is greater vibrational energy, and the 2nd set of conditions, greater translational energy. &lt;br /&gt;
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According to Polanyi&#039;s Rules, we would expect this reaction to be best activated by vibrational energy. The two graphs below agree with these findings. &lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.32.46.png|thumb|upright|330x330px|Contour plot for greater vibrational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.33.04.png|thumb|upright|330x330px|Contour plot for greater translational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794069</id>
		<title>013366322</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794069"/>
		<updated>2019-06-03T11:50:42Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Q2 - 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;== EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system  ==&lt;br /&gt;
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====&#039;&#039;&#039;Q1 - 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?&#039;&#039;&#039;====&lt;br /&gt;
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On the potential energy surface, the transition state is the position along the minimum energy pathway, linking reactants and products, where potential is highest. The transition structure exists at a saddle point of the potential energy surface - that is when ∂V(&#039;&#039;&#039;ri&#039;&#039;&#039;)/∂(&#039;&#039;&#039;ri&#039;&#039;&#039;)=0. Furthermore, the 2nd partial derivatives with respect to the orthogonal vectors r1 and r2 have opposite signs; one is positive and the other negative. This tells us that this is a saddle point.&lt;br /&gt;
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[[File:Screenshot_2019-05-21_at_14.27.22.png|400px]]&lt;br /&gt;
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{{fontcolor|pink|Be careful to makesure you say &amp;quot;potential energy&amp;quot; not just &amp;quot;potential&amp;quot;. And yes this is all correct and clearly explained but you are missing part of the definition. The TS is a saddle point because it is the maximum along the reaction trajectory and a minimum in the orthogonal direction, so which vector r1 or r2 will be positive or negative? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:47, 3 June 2019 (BST)}}&lt;br /&gt;
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====&#039;&#039;&#039;Q2 - 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.&#039;&#039;&#039;====&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 14.41.20.png|thumb|upright|400x400px|A graph showing Intermolecular distance Vs Time ]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_16.25.22.png|thumb|upright|400x400px|Contour Plot to find rts]]&lt;br /&gt;
|}&lt;br /&gt;
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Firstly, we set AB=BC and momentum equal to 0. Then, plotting a graph of Internuclear Distance vs Time, we can find the transition state. The optimised distance is the distance at which there is no trajectory towards either reactants or products and at which oscillations are reduced producing a straight line as seen in the plot above. As the graph shows straight lines, we know there is no vibration, and the atoms stop moving. That is, potential energy is maximum and kinetic energy zero. As such, the optimised distance is found to be 0.9079 Å. Looking at the contour plot above, the transition state can also be seen in approximately the correct location, backing up the result.&lt;br /&gt;
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{{fontcolor|pink|Great explanation - very clear and well understood.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:50, 3 June 2019 (BST)}}&lt;br /&gt;
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====&#039;&#039;&#039;Q3 - Comment on how the MEP and the trajectory you just calculated differ.&#039;&#039;&#039;====&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_15.06.08.png|thumb|upright|400x400px|MEP Calculation]]&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 15.07.56.png|thumb|upright|400x400px|Dynamics Calculation]]&lt;br /&gt;
|}&lt;br /&gt;
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The MEP graph shows no molecular vibration (as velocity=0) with momentum being equal to 0 in every time step. In comparison, the dynamics plot shows the vibrational energy of the molecule as seen by the non-straight line.&lt;br /&gt;
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===&#039;&#039;&#039;Q4 - 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?&#039;&#039;&#039;===&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; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the trajectory !! Description of the dynamics &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || YES || [[File:Screenshot_dex_1.png|400x400px]] || Both reactants collide and have sufficient energy to surpass the activation barrier. Products are formed. Vibrational motion is also seen evident by the oscillations.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0  || -100.456 || NO || [[File:Screenshot_dex_2.png|400x400px]] || Atom C collides molecule AB but has insufficient kinetic energy to overcome the activation energy, thus not forming products. Molecules do not pass through the transition state.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5  || -98.956 || YES || [[File:Screenshot_dex_3.png|400x400px]] || Both molecules have sufficient energy to surpass the activation energy and so pass though the transition state, forming the products.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0  || -84.956 || NO || [[File:Screenshot_dex_4.png|400x400px]] || Both molecules have large energies and are able to overcome the activation energy. However, their energy is so great, that they recross the barrier and reform reactants.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2  || -83.416 || YES || [[File:Screenshot_dex_5.png|400x400px]] || Both molecules have sufficient energy to overcome the activation energy barrier, but have the potential to cross back over the barrier, and reform products. &lt;br /&gt;
|}&lt;br /&gt;
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It can be concluded that if reactants do not have sufficient kinetic energy to surpass the activation barrier, then the reaction will not occur. Furthermore, if the reactants have an excess of kinetic energy, the reaction also may not proceed as the products formed turn back into reactants.&lt;br /&gt;
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===&#039;&#039;&#039;Q5 - State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Electron and nuclear motion are independent&lt;br /&gt;
Energy of the particles follows the Boltzmann distribution&lt;br /&gt;
Once reactants begin to combine and form the transition state, the transition state structure does not collapse to form reactants again&lt;br /&gt;
&lt;br /&gt;
Theory states that transition state structure does not collapse to reform the reactants. However, as experimental procedure shows, this can occur. As theory assumes that all reactions with sufficient energy will go onto form products, the real rate of reaction is much slower than in theory as reactants can be reformed. &lt;br /&gt;
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== EXERCISE 2: F - H - H system ==&lt;br /&gt;
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===&#039;&#039;&#039;Q6 - 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?&#039;&#039;&#039;===&lt;br /&gt;
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 {|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_dex_f_h2.png|thumb|upright|400x400px|Surface Plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_dex_h_hf.png|thumb|upright|400x400px|Surface Plot for H + HF]]&lt;br /&gt;
|}&lt;br /&gt;
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As seen above, the surface plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; starts at a high energy position dropping down lower energy after the transition state. Therefore, this is an exothermic reaction. In contrast, for the surface plot of HF + H, the reaction starts at a low energy position and needs a large amount of energy to over come the activation energy barrier. After passing the transition state, the energy falls a small amount. This reaction is therefore endothermic. From this, we can conclude that the HF bond is stronger than the HH bond since HF is lower in energy than HH. &lt;br /&gt;
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Furthermore, Hammond&#039;s Postulate states that the transition state will resemble either the product or reactants, whichever it is closer to in energy. To find the transition state, optimisation was completed as before with both momenta set to zero. Optimisation was completed so that there was minimal oscillation (gradient of line =0) seen for the Internuclear Distance vs Time graph, as shown below. The optimised distances were found to be r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-F)=1.813 Å and r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-H)=0.7445 Å. &lt;br /&gt;
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[[File:Screenshot_2019-05-21_at_18.21.10.png|thumb|upright|400x400px|Graph showing Internuclear Distance vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
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===&#039;&#039;&#039;Q7 - Report the activation energy for both reactions.&#039;&#039;&#039;===&lt;br /&gt;
Below shows two graphs depicting the total energy plot of both reactions. The activation energy for both reactions can be calculated as the difference between the highest and lowest energy levels. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.37.01.png|500px|left|thumb|Graph of Energy vs Steps for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.41.09.png|500px|right|thumb|Graph of Energy vs Steps for HF + H.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(H + HF)&#039;&#039;&#039;= +31.22 kcalmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)&#039;&#039;&#039;= +0.130 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q8 - 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.&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; a reactive trajectory was found using the following set of initial conditions: AB = 0.74 Å, BC = 1.80 Å, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5, and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.70. Using these intial conditions the graph of Momentum vs Time was produced, as seen below.&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.01.png|thumb|upright|400x400px|Graph of Momentum vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.11.png|thumb|upright|400x400px|Graph of Energy vs Time ]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
As you can see, whenever potential energy is lost, kinetic energy is gained by the same amount. Due to the exothermic nature of this reactrion, this kinetic energy is then converted into heat and can experimentally be seen by the increase in temperature.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q9 - 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.&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s Rule states that vibrational energy is much less successful in promoting an early transition state than translational energy is. Additionally, the opposite is true - translational energy is more efficient in promoting a late transition state than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
As seen above when calculating the activation energy of reaction, the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Hammond&#039;s Postulate states that this reaction therefore has an early transition state. Using Polanyi&#039;s Rules, this reaction would be most effectively activated by translational energy. Similarly, for the reaction of H + HF (endothermic), this would be most efficiently activated by vibrational energy.&lt;br /&gt;
&lt;br /&gt;
For the first reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, I used the values of r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.74 Å, and r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=1.81 Å.  Then i looked at the contour plots for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-2.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-0.5 (Left diagram), and for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-2.5 (right diagram). For the initial set of conditions, there is greater vibrational energy, and the 2nd set of conditions, greater translational energy. &lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s Rules, we would expect this reaction to be best activated by vibrational energy. The two graphs below agree with these findings. &lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.32.46.png|thumb|upright|330x330px|Contour plot for greater vibrational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.33.04.png|thumb|upright|330x330px|Contour plot for greater translational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794068</id>
		<title>013366322</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=013366322&amp;diff=794068"/>
		<updated>2019-06-03T11:47:30Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Q1 - 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&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system  ==&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q1 - 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?&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
On the potential energy surface, the transition state is the position along the minimum energy pathway, linking reactants and products, where potential is highest. The transition structure exists at a saddle point of the potential energy surface - that is when ∂V(&#039;&#039;&#039;ri&#039;&#039;&#039;)/∂(&#039;&#039;&#039;ri&#039;&#039;&#039;)=0. Furthermore, the 2nd partial derivatives with respect to the orthogonal vectors r1 and r2 have opposite signs; one is positive and the other negative. This tells us that this is a saddle point.&lt;br /&gt;
&lt;br /&gt;
[[File:Screenshot_2019-05-21_at_14.27.22.png|400px]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Be careful to makesure you say &amp;quot;potential energy&amp;quot; not just &amp;quot;potential&amp;quot;. And yes this is all correct and clearly explained but you are missing part of the definition. The TS is a saddle point because it is the maximum along the reaction trajectory and a minimum in the orthogonal direction, so which vector r1 or r2 will be positive or negative? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:47, 3 June 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q2 - 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.&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 14.41.20.png|thumb|upright|400x400px|A graph showing Intermolecular distance Vs Time ]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_16.25.22.png|thumb|upright|400x400px|Contour Plot to find rts]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Firstly, we set AB=BC and momentum equal to 0. Then, plotting a graph of Internuclear Distance vs Time, we can find the transition state. The optimised distance is the distance at which there is no trajectory towards either reactants or products and at which oscillations are reduced producing a straight line as seen in the plot above. As the graph shows straight lines, we know there is no vibration, and the atoms stop moving. That is, potential energy is maximum and kinetic energy zero. As such, the optimised distance is found to be 0.9079 Å. Looking at the contour plot above, the transition state can also be seen in approximately the correct location, backing up the result.&lt;br /&gt;
&lt;br /&gt;
====&#039;&#039;&#039;Q3 - Comment on how the MEP and the trajectory you just calculated differ.&#039;&#039;&#039;====&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_15.06.08.png|thumb|upright|400x400px|MEP Calculation]]&lt;br /&gt;
| [[File:Screenshot 2019-05-21 at 15.07.56.png|thumb|upright|400x400px|Dynamics Calculation]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The MEP graph shows no molecular vibration (as velocity=0) with momentum being equal to 0 in every time step. In comparison, the dynamics plot shows the vibrational energy of the molecule as seen by the non-straight line.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q4 - 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?&#039;&#039;&#039;===&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; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Illustration of the trajectory !! Description of the dynamics &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.018 || YES || [[File:Screenshot_dex_1.png|400x400px]] || Both reactants collide and have sufficient energy to surpass the activation barrier. Products are formed. Vibrational motion is also seen evident by the oscillations.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0  || -100.456 || NO || [[File:Screenshot_dex_2.png|400x400px]] || Atom C collides molecule AB but has insufficient kinetic energy to overcome the activation energy, thus not forming products. Molecules do not pass through the transition state.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5  || -98.956 || YES || [[File:Screenshot_dex_3.png|400x400px]] || Both molecules have sufficient energy to surpass the activation energy and so pass though the transition state, forming the products.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0  || -84.956 || NO || [[File:Screenshot_dex_4.png|400x400px]] || Both molecules have large energies and are able to overcome the activation energy. However, their energy is so great, that they recross the barrier and reform reactants.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2  || -83.416 || YES || [[File:Screenshot_dex_5.png|400x400px]] || Both molecules have sufficient energy to overcome the activation energy barrier, but have the potential to cross back over the barrier, and reform products. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
It can be concluded that if reactants do not have sufficient kinetic energy to surpass the activation barrier, then the reaction will not occur. Furthermore, if the reactants have an excess of kinetic energy, the reaction also may not proceed as the products formed turn back into reactants.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q5 - State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Electron and nuclear motion are independent&lt;br /&gt;
Energy of the particles follows the Boltzmann distribution&lt;br /&gt;
Once reactants begin to combine and form the transition state, the transition state structure does not collapse to form reactants again&lt;br /&gt;
&lt;br /&gt;
Theory states that transition state structure does not collapse to reform the reactants. However, as experimental procedure shows, this can occur. As theory assumes that all reactions with sufficient energy will go onto form products, the real rate of reaction is much slower than in theory as reactants can be reformed. &lt;br /&gt;
&lt;br /&gt;
== EXERCISE 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q6 - 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?&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
 {|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_dex_f_h2.png|thumb|upright|400x400px|Surface Plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_dex_h_hf.png|thumb|upright|400x400px|Surface Plot for H + HF]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
As seen above, the surface plot for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; starts at a high energy position dropping down lower energy after the transition state. Therefore, this is an exothermic reaction. In contrast, for the surface plot of HF + H, the reaction starts at a low energy position and needs a large amount of energy to over come the activation energy barrier. After passing the transition state, the energy falls a small amount. This reaction is therefore endothermic. From this, we can conclude that the HF bond is stronger than the HH bond since HF is lower in energy than HH. &lt;br /&gt;
&lt;br /&gt;
Furthermore, Hammond&#039;s Postulate states that the transition state will resemble either the product or reactants, whichever it is closer to in energy. To find the transition state, optimisation was completed as before with both momenta set to zero. Optimisation was completed so that there was minimal oscillation (gradient of line =0) seen for the Internuclear Distance vs Time graph, as shown below. The optimised distances were found to be r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-F)=1.813 Å and r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;(H-H)=0.7445 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:Screenshot_2019-05-21_at_18.21.10.png|thumb|upright|400x400px|Graph showing Internuclear Distance vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
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===&#039;&#039;&#039;Q7 - Report the activation energy for both reactions.&#039;&#039;&#039;===&lt;br /&gt;
Below shows two graphs depicting the total energy plot of both reactions. The activation energy for both reactions can be calculated as the difference between the highest and lowest energy levels. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.37.01.png|500px|left|thumb|Graph of Energy vs Steps for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
![[File:Screenshot_2019-05-24_at_16.41.09.png|500px|right|thumb|Graph of Energy vs Steps for HF + H.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(H + HF)&#039;&#039;&#039;= +31.22 kcalmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Activation Energy(F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)&#039;&#039;&#039;= +0.130 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q8 - 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.&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; a reactive trajectory was found using the following set of initial conditions: AB = 0.74 Å, BC = 1.80 Å, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5, and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -1.70. Using these intial conditions the graph of Momentum vs Time was produced, as seen below.&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.01.png|thumb|upright|400x400px|Graph of Momentum vs Time for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-21_at_18.43.11.png|thumb|upright|400x400px|Graph of Energy vs Time ]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
As you can see, whenever potential energy is lost, kinetic energy is gained by the same amount. Due to the exothermic nature of this reactrion, this kinetic energy is then converted into heat and can experimentally be seen by the increase in temperature.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Q9 - 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.&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s Rule states that vibrational energy is much less successful in promoting an early transition state than translational energy is. Additionally, the opposite is true - translational energy is more efficient in promoting a late transition state than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
As seen above when calculating the activation energy of reaction, the reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Hammond&#039;s Postulate states that this reaction therefore has an early transition state. Using Polanyi&#039;s Rules, this reaction would be most effectively activated by translational energy. Similarly, for the reaction of H + HF (endothermic), this would be most efficiently activated by vibrational energy.&lt;br /&gt;
&lt;br /&gt;
For the first reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, I used the values of r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.74 Å, and r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=1.81 Å.  Then i looked at the contour plots for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-2.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-0.5 (Left diagram), and for when &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 and &#039;&#039;&#039;p&#039;&#039;&#039;&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-2.5 (right diagram). For the initial set of conditions, there is greater vibrational energy, and the 2nd set of conditions, greater translational energy. &lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s Rules, we would expect this reaction to be best activated by vibrational energy. The two graphs below agree with these findings. &lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.32.46.png|thumb|upright|330x330px|Contour plot for greater vibrational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
| [[File:Screenshot_2019-05-24_at_13.33.04.png|thumb|upright|330x330px|Contour plot for greater translational energy - F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:24970&amp;diff=793690</id>
		<title>MRD:24970</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:24970&amp;diff=793690"/>
		<updated>2019-05-28T11:25:11Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Exercise 2: F-H-H System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; Molecule ==&lt;br /&gt;
&lt;br /&gt;
===Dynamics from the transition state region===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is defined as the maximum point on the lowest energy path between reactants and products where the first partial derivative      (∂V/∂r) is equal to 0 and the second derivative, (∂V&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/dr&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;) , is positive. It can be distinguished from a local minimum as it satisfies the condition that ∂V/dq&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0 and ∂V/dq&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, where q1 is the tangent at the minimum of a reaction pathway and q2 is a line at right-angles to this tangent.&lt;br /&gt;
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{{fontcolor|pink|This isn&#039;t quite right mathematically. As the transition state is the maximum point on the lowest energy pathway, the second partial derivative in the direction of the lowest energy pathway is negative, as the second partial derivative of a maximum is negative. As the transition state is a point on the lowest energy pathway, it is a minimum in the direction that is orthogonal to the reaction trajectory and therefore in that direction the second partial derivative is positive because the second partial derivative of a minimum is positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 10:45, 28 May 2019 (BST)}}&lt;br /&gt;
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&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The best estimate for the transition state position is where 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; are 0.9075Å because at this inter-atomic distance, the atoms are static and not vibrating. In the Internuclear Distance vs Time plot, the distance remains the same over time.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|I can see what you are getting at but you need to provide a much more in depth explanation of what you are trying to say. For example, you need to explain why atoms not vibrating means that you have found the TS. The reason is that as the molecule approaches the TS (increases in E on the potential surface) it gains potential energy and therefore it must lose vibrational energy due to conservation of energy. Again, what do you mean by the internuclear distances remaining the same over time? Specify a time frame, and specify why this means you are at the TS. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 10:45, 28 May 2019 (BST)}}&lt;br /&gt;
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[[File:Transition_state_sk.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The trajectory calculated by MEP differs from the one calculated by Dynamics as it does not oscillate, whereas the one calculated by Dynamics does. This means that the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is vibrating as it moves away from the  hydrogen atom , whereas in the MEP it is not. Another difference is that in the MEP calculation , the trajectory stops at the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; distance of 2.25Å whereas it continues to infinity in the Dynamics calculation.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|But why does the MEP not oscillate but the Dynamics calculation does? Do you understand the difference between them on the level of the calculation? This is important to demonstrate. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 10:45, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !!E&amp;lt;sub&amp;gt;tot &amp;lt;/sub&amp;gt;(kcal/mol)!! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  ||-99.018||Yes||C approaches molecule A-B, a reaction occurs &lt;br /&gt;
forming molecule B-C, which moves away from A while vibrating.&lt;br /&gt;
&lt;br /&gt;
|| [[File:trajectory1_sk.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  || -100.456 &lt;br /&gt;
|| No  &lt;br /&gt;
|| C approaches molecule A-B but doesn&#039;t react, causing C &lt;br /&gt;
to move away from A-B.&lt;br /&gt;
|| [[File:trajectory2_sk.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  || -98.956&lt;br /&gt;
|| Yes&lt;br /&gt;
|| C approaches vibrating molecule A-B, a reaction occurs forming molecule&lt;br /&gt;
B-C, which moves away from A while vibrating.&lt;br /&gt;
|| [[File:trajectory3_sk.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  || -84.956&lt;br /&gt;
|| No&lt;br /&gt;
|| C approaches A-B and a transition state is reached. However,&lt;br /&gt;
the original reactants reform and C moves away from A-B.&lt;br /&gt;
|| [[File:trajectory4_sk.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  || -83.416&lt;br /&gt;
|| Yes&lt;br /&gt;
|| C approaches A-B, a transition state is reached and for a brief period, &lt;br /&gt;
it seems like the original reactants reform. However,the transition state&lt;br /&gt;
&lt;br /&gt;
is passed over again and a molecule of B-C is formed.&lt;br /&gt;
|| [[File:trajectory5_sk.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
One can conclude from the above table that the total energy of a reaction is determined by the momentum of the reacting particles, which is related to their kinetic energies. However, the success of the reaction is determined not by the total energy of the reaction, but by the relative momentum values of 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;.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This is a fairly insightful conclusion. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 10:51, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Transition theory states that in a reaction between A and B molecules, an activated complex C is formed that is in equilibrium with the reactants and is at a greater energy than both reactants and products. The prediction of reaction rate by Transition State Theory will be a greater value than that predicted by experiment as it is shown in the penultimate reaction in the table that a reaction can be unsuccessful if barrier recrossing occurs, even if the reacting particles have an energy greater than the activation energy.&amp;lt;ref&amp;gt;Peter Atkins. Judio De Paula. Atkins Physical Chemistry (Ninth Edition). Oxford: Oxford University Press; 2001.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| The discussed theory is called transition state theory, not transition theory. You have partially answered the question but you were asked to state 3 assumptions made by the theory. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 10:51, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F-H-H System ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as the potential surface shows that the products have a lower energy than the reactants. Hence, the reverse reaction to this ( H + HF) must be endothermic as the products are higher in energy than the reactants. The process of bond making is exothermic and as the reaction of F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to form HF is exothermic and this involves making a H-F bond and breaking a H-H bond, we can conclude that the H-F bond is stronger than the H-H bond.&lt;br /&gt;
&lt;br /&gt;
[[File:Fluorine_SK.png|300px]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The H-H distance in the transition state is 0.745 Å while the H-F distance is 1.808 Å. The contour plot at these inter-nuclear distances show that there is no reaction trajectory.&lt;br /&gt;
&lt;br /&gt;
[[File:HF_sk.png|300px]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy for the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F → HF + H is 0.2 kcal/mol as the transition state has an energy of -103.742 kcal/mol and the reactants have an energy of -103.911 kcal/mol. For the reaction HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F, the activation energy has a value of 30 kcal/mol as the reactants lie at -133.864 kcal/mol.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Where did you get these numbers? It is important in questions like this that you demonstrate your understanding by showing how you find energies etc. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 10:56, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The mechanism  involves translational energy being converted to vibrational energy, upon collison between the molecule and atom. To measure the release of vibrational energy, an infa-red spectrum could be experimentally recorded whereas the translational energy could be measured using bomb calorimetry, which provides a measure of the kinetic energy&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| What exactly does calorimetry measure and how can that be applied in terms of energy? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 10:56, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|+&lt;br /&gt;
!p&amp;lt;sub&amp;gt;HH &amp;lt;/sub&amp;gt;value&lt;br /&gt;
!Reactive?&lt;br /&gt;
!H-H Bond Vibration Level&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|Very Strong&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.95&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|Strong&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.9&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|Strong&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|Strong&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|Strong&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|Medium&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|Medium&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|Weak&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-0.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|Very weak&lt;br /&gt;
|-&lt;br /&gt;
|0&lt;br /&gt;
|Yes&lt;br /&gt;
|Very weak&lt;br /&gt;
|-&lt;br /&gt;
|0.5&lt;br /&gt;
|No&lt;br /&gt;
|Very weak&lt;br /&gt;
|-&lt;br /&gt;
|1&lt;br /&gt;
|No&lt;br /&gt;
|Weak&lt;br /&gt;
|-&lt;br /&gt;
|1.5&lt;br /&gt;
|No&lt;br /&gt;
|Medium&lt;br /&gt;
|-&lt;br /&gt;
|2&lt;br /&gt;
|No&lt;br /&gt;
|Medium&lt;br /&gt;
|-&lt;br /&gt;
|2.5&lt;br /&gt;
|No&lt;br /&gt;
|Strong&lt;br /&gt;
|-&lt;br /&gt;
|2.85&lt;br /&gt;
|Yes&lt;br /&gt;
|Strong&lt;br /&gt;
|-&lt;br /&gt;
|2.9&lt;br /&gt;
|Yes&lt;br /&gt;
|Strong&lt;br /&gt;
|-&lt;br /&gt;
|2.95&lt;br /&gt;
|Yes&lt;br /&gt;
|Strong&lt;br /&gt;
|-&lt;br /&gt;
|3&lt;br /&gt;
|No&lt;br /&gt;
|Strong&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
This table shows how changing the momentum of the hydrogen molecule p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has effect on whether the reaction H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F → HF + H will occur. The values of p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; is -0.5 and the H-H and H-F distances are 0.74 and 1.81 respectively. The reaction is successful when the momentum value is between 0-2, and 2.85 and 2.95. This shows that there isn&#039;t an obvious relationship between the momentum value and whether the reaction will be successful.&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is changed to 0.1 and p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; is changed to -0.8, it is observed that the reaction is still successful.&lt;br /&gt;
&lt;br /&gt;
[[File:momentum_sk.png|300px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi’s empirical rules state that for an early transition state, like in an exothermic reaction, translational energy has a greater effect than vibrational energy on the efficiency of reaction. On the contrary, endothermic reactions that have a late transition state depend more on the vibrational energy.&amp;lt;ref&amp;gt;2) J.C.Polanyi. Energy Distribution Among Reagents and Products of Atomic Reactions. &#039;&#039;J. Chem. Phys&#039;&#039;. 31, 1338 (1959). Available from: https://doi.org/10.1063/1.1730597 [Accessed 20th May 2019]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Try to be more explicit: in an early TS system, high translational energy will make the system reactive and high vibrational will not, and vice versa. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 10:56, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Due to the exothermic nature of the reaction F + H2 → HF + H, this suggests that the efficiency of the reaction depends more on the translational energy. The H-F momentum represents the translational energy while the H-H momentum represents the vibrational energy. Hence it its predicted that increasing the H-F momentum will have a greater effect in making the reaction go to completion whereas increasing the H-H momentum would have the opposite effect. The table above demonstrates that as the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; was increased from -1 and -3, the reaction became unsuccessful as there was an increase in H-H vibrational energy.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793689</id>
		<title>MRD:MToth96</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793689"/>
		<updated>2019-05-28T11:23:39Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /*  Q5 Polanyi&amp;#039;s Empirical Rule and the Distribution of Energy  */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Collision of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Potential Energy Surface&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
 [[File:Surface_Plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface (&#039;&#039;see above&#039;&#039;), the transition state is found and defined as the point where it is true that ∂V(ri)/∂ri=0, and ∂V2(ri)/∂ri2&amp;gt;0.                       &lt;br /&gt;
Empirically, the gradient of the surface is hence equals zero. Looking at the surface plot, the kinetic energy surface, as a function of AB distance has &lt;br /&gt;
a curvature that describes the potential energy as a function of distance. The transition state is at its minimum, as the distances are in balance. &lt;br /&gt;
Also, the trajectory (see black line) has to have its maximum value at the transition state, as we are expecting an energy maximum at this point. &lt;br /&gt;
The transition state is the highest point along the trajectory. At this point, AB and BC are also equal. After the second differentiation, a local maximum &lt;br /&gt;
is found if the derived value is positive. It is distinguished from other local minima by implementing the following criterium: ∂V/dq1 = 0 and ∂V/dq2 = 0, &lt;br /&gt;
where q1 is the tangent to the minimum and q2 is orthogonal to this as well as to the reaction path. Hence, ∂V2/dq12 &amp;lt; 0 and ∂V2/dq22 &amp;gt; 0 for that point.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This isn&#039;t quite correct. The transition state is both a maximum and a minimum, in different directions. In the direction of the minimum energy trajectory (i.e. the path the black line follows) it is a maximum. The second partial derivative of a maximum is always negative. Therefore the second partial derivative of the function of the PES in the direction of the reaction trajectory will be negative. However, as the TS occurs on the minimum energy pathway, this point is also a minimum, but in a direction orthogonal to the reaction trajectory. Therefore, as the second partial derivative of a minimum is always positive, the second partial derivative of the PES at the TS in the direction orthogonal to the trajectory will be positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:04, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Locating Transition States&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
When the transition state is reached, both the AB and BC distances are equal. Atoms show no vibration and therefore the graph displays no straight lines in accordance with this observation. The optimal distance was found to be 0.908 Å, at which both AB and BC distances were equal. Also, the momentum for both p1 and p2 were set to zero. &lt;br /&gt;
The Intermolecular distanced vs Time plot is shown below (on the left). The aim was to minimise oscillation and obtain flat lines with no corresponding gradients. No vibration means no change in distance and the vibration of the H atom and molecule is restricted. A restriction in vibrational freedom means that the TS is reached. Moreover, the BC and AB distances are equal and the corresponding lines are on top of each other. A static picture of the animation of the transition state can be seen below (on the right)&lt;br /&gt;
&lt;br /&gt;
[[File:Diastance_vs_time_h2.PNG]] .     [[File:Animation_h2_static.PNG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Why does a restriction in vibrational freedom mean that the TS is reached? Also be careful - the distance AB=BC at the TS only for a symmetrical reaction and that is only because reactants = products. This is not true of any TS. Perhaps you are aware of this, but you need to state it explicitly in order for this statement to be true. I also do not understand your point stating that &amp;quot;the graph displays no straight lines&amp;quot; where there is no vibration. What straight lines? In order to be very clear about what you mean, you need to explain every point you make thoroughly.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:07, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 MEP and Dynamic Trajectory&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_mep.PNG]] .     [[File:Surface_dynamic.PNG]]&lt;br /&gt;
&lt;br /&gt;
The trajectory is displayed as the black line along the bottom of the surface plots (&#039;&#039;see above&#039;&#039;. When the MEP calculation (on the left) is used, the line starts from the transition state but is only displayed for a short length. Whereas, the dynamic calculation (on the right) gives a much longer, complete black trajectory. The program tries to find the steepest descent along the potential energy surface to obtained a minimum. The MEP method is being reset to zero after every step, whilst with dynamic calculation the data is being carried further to the next step. Hence, the calculation is being carried on regardless, whereas with MEP the kinetic energy stays at its minimum. Thus, an oscillating line with the dynamic, and a local maximum with the MEP calculation is being observed. &lt;br /&gt;
&lt;br /&gt;
[[File:normal.PNG]]               [[File:Changed_distance.PNG]]&lt;br /&gt;
&lt;br /&gt;
For comparison, values of interatomic distances were changed (&#039;&#039;see above&#039;&#039;. Values were being shifted from r1=ts+0.01, r2=ts (on the left); to r1=ts and r2=ts+0.01 (on the right)&lt;br /&gt;
In both cases, it was observed that the lines corresponding to the AB and BC distances were exchanged (as expected). When the numbers got changed, the transition state was approached by the opposite direction - as a symmetrical system is being considered - and the values are exactly the same but opposite. Hence, the same plot was displayed in the opposite direction. The same variations were applied for Momenta vs Time plots. The observations are exactly the same as for the distances, with the position of the lines being exchanged in between. The initial values are displayed below on the left, whereas the changed values can be seen on the right.&lt;br /&gt;
&lt;br /&gt;
[[File:Normal_momentum.PNG]]         [[File:Changed.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Reactivity through trajectory analysis &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; (kcal.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;
| -1.25 || -2.5  || -99.018 || Yes || A-B oscillates, B and C bond formation || [[File:-1.25,-2.5_p1,p2.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  || -100.456 || No || A-B oscillates, no reaction || [[File:-1.5,-2.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  || -98.956 || Yes || A-B oscillates, B and C bond formation || [[File:-1.5,-2.5.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  || -84.956 || No ||  A-B oscillates intensely, B and C bond formation is expected, but it bounces off and C remains a single atom || [[File:-2.5,-5.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  || -83.416 || Yes || 	A-B oscillates intensely, very close transition state, B and C bond formation || [[File:-2.5,-5.2.png]]&lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
From the table above it was concluded that the E total of the system depends on the momentum. Moreover, it shows a correlation with the kinetic energy of the system. The potential energy is constant and the kinetic energy is changing in response the structural changes. Furthermore, the system&#039;s susceptibility to undergo a reaction is also dependent on the momentum (not just on energy). If there is a large momentum difference between the single atom and the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule - especially when the incoming atom&#039;s momentum is marginally lower - than the reaction will not happen.&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5  Transition State Theory &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Transition State theory&amp;lt;ref name=&amp;quot;No.1&amp;quot; /&amp;gt; is a way of describing chemical reactions as such that the reaction consist of atoms and molecules are subjected to a continuous change in the energies and positions. The transition state is being described as the position along the reaction path where the energy is at its maximum. The activation energy corresponding to a specific reaction and to its reactant is the energy necessary to initiate collisions sufficient to reach the transition state. It is calculated as the difference between the reactants and the transition state. The transition state or activated complex is in equilibrium with the reactant and hence its properties can be approximated using Hammond&#039;s postulate. Moreover, the rate if reaction - formation of products - can be approximates from the concentration of these activated complexes and their ability to go to completion.&lt;br /&gt;
&lt;br /&gt;
Furthermore, the transition state theory can also be applied to the quasi-equilibrium state. The reactants are in equilibrium with the transition state complex. This means that an equilibrium is always established in between the reactant and the activated complex regardless of the relationship of the reactant and the product (if they are in equilibrium). This part of the theory can be materialised in the form of a mathematical expression through the Van Hoff equation. The equation describes an equilibrium state, which is reversible and temperature dependent. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{d\ln K}{dT} = \frac{\Delta U}{RT^{2}}&amp;lt;/math&amp;gt;    &#039;&#039;where, K - eq. constant, T - temperature in K, U - internal energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In order to get the temperature dependence of reaction rates, the equation is derived and as a result the Arrhenius equation is being formulated. The Arrhenius equation shows the temperature dependence of reaction rates as well as the activation energy of a corresponding reaction.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;k = Ae^{-E_a/RT}&amp;lt;/math&amp;gt;     &#039;&#039;where k - rate constant, T - temperature in K, A - exponential factor, Ea - activation energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
According to the theory, the last reaction -  where P1 and P2 were -2.5 and -5.0 respectively - must go to completion. However, the exact opposite was observed. As a conclusion, it is suggested that the rate constant is lower in real life than it is in theory. Therefore, the rate constant prevents the reaction from going to completion. (the energy barrier is sufficient to retain AB as a molecule when is it being subjected to a collision by C)&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This is sort of the right idea but a bit confused! Yes, TST states that once a reaction has reached the TS and crossed over to the product side, it will not cross back to the reactant side (the assumption of TST is the idea of no barrier recrossing). However in real life barrier recrossing can occur. Therefore the rate constant will be overpredicted by TST, as you have said. However, the rate constant does not prevent the reaction from going to completion and I cannot quite understand what you mean by this point. The main idea is there though. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:14, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;System of F-H-H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Classification of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:FH_E_surface.png]]&lt;br /&gt;
&lt;br /&gt;
Atoms A and B are H-s, whereas C was F. The surface plot (&#039;&#039;see above&#039;&#039;) shows that the reactants (on the right hand side) are higher in energy than the product (on the left hand side). Therefore the reaction:&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H &lt;br /&gt;
&lt;br /&gt;
is exothermic (negative sign, accompanied by a decrease in energy). Hence the reverse reaction: &lt;br /&gt;
&lt;br /&gt;
H + HF → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F&lt;br /&gt;
&lt;br /&gt;
must be endothermic, as this is the corresponding backward reaction. In that case, the reactants will be lower in energy and the products will be higher. Additional energy is required to pass the activation energy barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:HF_surfce_endothemic.png]] &lt;br /&gt;
&lt;br /&gt;
The first reaction is exothermic, (bond making is exothermic) which means that the final product will be in a lower energy state than the reactants. Hence, the HF bond is a stronger bond and is lower in energy than the H-H bond. This is due to the ionic nature of the H-F bond due to a large difference in electronegativity. The surface plot of the endothermic reaction is shown above. It can be depicted that the reactant are in a lower energy state than the product.&lt;br /&gt;
For these calculations p1=p2=0&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Really good answer. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:16, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Position of the Transition State&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_plot_norxn.png]]      [[File:Contour_norxn.png]]&lt;br /&gt;
&lt;br /&gt;
To find the transition state, the surface (above, on the left) and contour (above, on the right) plots were displayed. At a transition state, only a single black dot can been seen on a surface plot as there is no trajectory. Moreover, the contour plot was left blank, as the reaction did not happen, but no oscillation is observed as the vibrational freedom of the complex is being retained. The transition state was obtained at H-H distance: 0.745 Å, and H-F distance: 1.808 Å.&lt;br /&gt;
&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 Activation Energies &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Using the Energy vs Time plots, the following values have been established:&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F → HF + H:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -103.913 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 0.226 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -132.455 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 28.768 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|You should show the plots as it is not clear how these values were obtained. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:17, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Mechanisms of energy release&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
A scenario was set up in which the Animation and Momenta vs Time plots show that the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; - F reaction goes to completion. B and C were the H and A was the F atoms, with distances of A-B 1.5 Å, and B-C 0.878 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:mom_vs_time_AB_1.5_BC_0.878.png]]&lt;br /&gt;
&lt;br /&gt;
When the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule collides with the F atom, the translational energy of the species (due to the attraction between them) is being transformed into vibrational energy (oscillation being observed). Depending on the nature of the experiment, exothermic reactions release whereas, endothermic reactions absorb energy (in the form of heat) from the environment. When the oscillating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (both) atom approaches the  F atom (only translational energy), oscillation in the form of vibrational energy is being transmitted to the residual HF molecule. This way, the energy of the system is constant but the vibrational and kinetic energies are being transformed in between species. This can be confirmed experimentally by measuring the vibrational energy of the system via IR spectroscopy or use bomb calorimetry to determine the kinetic energy of the system  - which is directly proportional to the translational energy and its momentum. &lt;br /&gt;
&lt;br /&gt;
rHH = 0.74 Å, with a momentum pFH = -0.5, pHH in the range -3 to 3, rHF was set to 1.5 Å&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! pHH !! Level of Vibration of H-H bond !! Reaction &lt;br /&gt;
|-&lt;br /&gt;
| -3 || medium || transition state &lt;br /&gt;
|-&lt;br /&gt;
| -2.9 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.8 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.7 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.6 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.25 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
|  -2|| medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| -1 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 0 || strong|| yes &lt;br /&gt;
|-&lt;br /&gt;
| 1 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 1.5 || weak || transition state &lt;br /&gt;
|-&lt;br /&gt;
|  2 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.25  || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.3 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.4 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.6 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.7 ||  weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
|  2.8 || weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| 2.9  || weak || yes  &lt;br /&gt;
|-&lt;br /&gt;
| 3 || medium || yes &lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction goes to completion between the values -1.5 and 1, 2.5-2.6 and 2.9-3.0. As a conclusion, it was determined that no certain trends can be depicted from the data which would link the momentum, the outcome and the stretch of vibrations together. Moreover, the reactions at 2.9 and 3.0 are against Polanyi&#039;s empirical rule.&lt;br /&gt;
&lt;br /&gt;
For a separate calculation, the same initial positions were used, for HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F  with rHH=0.74 A but the momentum of HF was changed to p= -0.8 and the HH momentum was 0.1. The reaction goes to completion and thus the reaction is valid!&lt;br /&gt;
&lt;br /&gt;
If we look at the Momenta vs Time plot, we can see a continuously oscillating path, hence the reaction had reached its end. A large momentum contribution is seen as a a result of a large contribution from the very strong HF bond. &lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; 2 Å&lt;br /&gt;
HF 0.893325 Å&lt;br /&gt;
Phh - 8&lt;br /&gt;
Phf -0,02&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|It would be best to include figures in the table to show the trajectory being reactive/unreactive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:22, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5 Polanyi&#039;s Empirical Rule and the Distribution of Energy &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Polany&#039;s empirical rules&amp;lt;ref name=&amp;quot;No.2&amp;quot; /&amp;gt; are reflecting on the effect of transition states energetically different modes. An exothermic reaction - in which the products are higher in energy - the transition state is described as &#039;early&#039; as it is closer in energy to the reactants. Hence, the translational energy has a greater impact on the activated complex snd thus the reaction then the vibrational energy. Empirically, for an endothermic reaction -  with a corresponding late transition state - the vibrational energy has a greater importance on the reaction.&lt;br /&gt;
&lt;br /&gt;
In this case, &lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H&lt;br /&gt;
&lt;br /&gt;
is an exothermic reaction. Therefore, as described above it has an early transition state which suggest a greater impact from the translational energy contribution. The vibrational energy can be seen through the oscillating nature of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, where the translational contribution is largely coming from the H-F bond (both can be seen through their momenta). The effect of HH momentum is low. Therefore, larger HF contribution (momentum) would increase the chances of the reaction being completed. The experiment has failed to show a specific trend which would also comply with the theory. The results at 2.9 and 3 violate Polanyi&#039;s rules as discussed in the previous question.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Your understanding of Polanyi&#039;s rules seems corrects, but it doesn&#039;t make sense that there would be a violation of Polanyi&#039;s rules in these simulations. However I cannot try to aid your understanding of it without a figure or description of the trajectory. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:23, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.1&amp;quot;&amp;gt;T. Bligaard, J.K. Nørskov, in Chemical Bonding at Surfaces and Interfaces, 2008&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.2&amp;quot;&amp;gt;Polanyi, J. C. Concepts in Reaction Dynamics Acc. Chem. Res. 1972, 5, 161– 168&amp;lt;/ref&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793688</id>
		<title>MRD:MToth96</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793688"/>
		<updated>2019-05-28T11:22:13Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /*  Q4 Mechanisms of energy release */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Collision of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Potential Energy Surface&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
 [[File:Surface_Plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface (&#039;&#039;see above&#039;&#039;), the transition state is found and defined as the point where it is true that ∂V(ri)/∂ri=0, and ∂V2(ri)/∂ri2&amp;gt;0.                       &lt;br /&gt;
Empirically, the gradient of the surface is hence equals zero. Looking at the surface plot, the kinetic energy surface, as a function of AB distance has &lt;br /&gt;
a curvature that describes the potential energy as a function of distance. The transition state is at its minimum, as the distances are in balance. &lt;br /&gt;
Also, the trajectory (see black line) has to have its maximum value at the transition state, as we are expecting an energy maximum at this point. &lt;br /&gt;
The transition state is the highest point along the trajectory. At this point, AB and BC are also equal. After the second differentiation, a local maximum &lt;br /&gt;
is found if the derived value is positive. It is distinguished from other local minima by implementing the following criterium: ∂V/dq1 = 0 and ∂V/dq2 = 0, &lt;br /&gt;
where q1 is the tangent to the minimum and q2 is orthogonal to this as well as to the reaction path. Hence, ∂V2/dq12 &amp;lt; 0 and ∂V2/dq22 &amp;gt; 0 for that point.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This isn&#039;t quite correct. The transition state is both a maximum and a minimum, in different directions. In the direction of the minimum energy trajectory (i.e. the path the black line follows) it is a maximum. The second partial derivative of a maximum is always negative. Therefore the second partial derivative of the function of the PES in the direction of the reaction trajectory will be negative. However, as the TS occurs on the minimum energy pathway, this point is also a minimum, but in a direction orthogonal to the reaction trajectory. Therefore, as the second partial derivative of a minimum is always positive, the second partial derivative of the PES at the TS in the direction orthogonal to the trajectory will be positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:04, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Locating Transition States&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
When the transition state is reached, both the AB and BC distances are equal. Atoms show no vibration and therefore the graph displays no straight lines in accordance with this observation. The optimal distance was found to be 0.908 Å, at which both AB and BC distances were equal. Also, the momentum for both p1 and p2 were set to zero. &lt;br /&gt;
The Intermolecular distanced vs Time plot is shown below (on the left). The aim was to minimise oscillation and obtain flat lines with no corresponding gradients. No vibration means no change in distance and the vibration of the H atom and molecule is restricted. A restriction in vibrational freedom means that the TS is reached. Moreover, the BC and AB distances are equal and the corresponding lines are on top of each other. A static picture of the animation of the transition state can be seen below (on the right)&lt;br /&gt;
&lt;br /&gt;
[[File:Diastance_vs_time_h2.PNG]] .     [[File:Animation_h2_static.PNG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Why does a restriction in vibrational freedom mean that the TS is reached? Also be careful - the distance AB=BC at the TS only for a symmetrical reaction and that is only because reactants = products. This is not true of any TS. Perhaps you are aware of this, but you need to state it explicitly in order for this statement to be true. I also do not understand your point stating that &amp;quot;the graph displays no straight lines&amp;quot; where there is no vibration. What straight lines? In order to be very clear about what you mean, you need to explain every point you make thoroughly.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:07, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 MEP and Dynamic Trajectory&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_mep.PNG]] .     [[File:Surface_dynamic.PNG]]&lt;br /&gt;
&lt;br /&gt;
The trajectory is displayed as the black line along the bottom of the surface plots (&#039;&#039;see above&#039;&#039;. When the MEP calculation (on the left) is used, the line starts from the transition state but is only displayed for a short length. Whereas, the dynamic calculation (on the right) gives a much longer, complete black trajectory. The program tries to find the steepest descent along the potential energy surface to obtained a minimum. The MEP method is being reset to zero after every step, whilst with dynamic calculation the data is being carried further to the next step. Hence, the calculation is being carried on regardless, whereas with MEP the kinetic energy stays at its minimum. Thus, an oscillating line with the dynamic, and a local maximum with the MEP calculation is being observed. &lt;br /&gt;
&lt;br /&gt;
[[File:normal.PNG]]               [[File:Changed_distance.PNG]]&lt;br /&gt;
&lt;br /&gt;
For comparison, values of interatomic distances were changed (&#039;&#039;see above&#039;&#039;. Values were being shifted from r1=ts+0.01, r2=ts (on the left); to r1=ts and r2=ts+0.01 (on the right)&lt;br /&gt;
In both cases, it was observed that the lines corresponding to the AB and BC distances were exchanged (as expected). When the numbers got changed, the transition state was approached by the opposite direction - as a symmetrical system is being considered - and the values are exactly the same but opposite. Hence, the same plot was displayed in the opposite direction. The same variations were applied for Momenta vs Time plots. The observations are exactly the same as for the distances, with the position of the lines being exchanged in between. The initial values are displayed below on the left, whereas the changed values can be seen on the right.&lt;br /&gt;
&lt;br /&gt;
[[File:Normal_momentum.PNG]]         [[File:Changed.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Reactivity through trajectory analysis &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; (kcal.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;
| -1.25 || -2.5  || -99.018 || Yes || A-B oscillates, B and C bond formation || [[File:-1.25,-2.5_p1,p2.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  || -100.456 || No || A-B oscillates, no reaction || [[File:-1.5,-2.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  || -98.956 || Yes || A-B oscillates, B and C bond formation || [[File:-1.5,-2.5.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  || -84.956 || No ||  A-B oscillates intensely, B and C bond formation is expected, but it bounces off and C remains a single atom || [[File:-2.5,-5.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  || -83.416 || Yes || 	A-B oscillates intensely, very close transition state, B and C bond formation || [[File:-2.5,-5.2.png]]&lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
From the table above it was concluded that the E total of the system depends on the momentum. Moreover, it shows a correlation with the kinetic energy of the system. The potential energy is constant and the kinetic energy is changing in response the structural changes. Furthermore, the system&#039;s susceptibility to undergo a reaction is also dependent on the momentum (not just on energy). If there is a large momentum difference between the single atom and the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule - especially when the incoming atom&#039;s momentum is marginally lower - than the reaction will not happen.&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5  Transition State Theory &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Transition State theory&amp;lt;ref name=&amp;quot;No.1&amp;quot; /&amp;gt; is a way of describing chemical reactions as such that the reaction consist of atoms and molecules are subjected to a continuous change in the energies and positions. The transition state is being described as the position along the reaction path where the energy is at its maximum. The activation energy corresponding to a specific reaction and to its reactant is the energy necessary to initiate collisions sufficient to reach the transition state. It is calculated as the difference between the reactants and the transition state. The transition state or activated complex is in equilibrium with the reactant and hence its properties can be approximated using Hammond&#039;s postulate. Moreover, the rate if reaction - formation of products - can be approximates from the concentration of these activated complexes and their ability to go to completion.&lt;br /&gt;
&lt;br /&gt;
Furthermore, the transition state theory can also be applied to the quasi-equilibrium state. The reactants are in equilibrium with the transition state complex. This means that an equilibrium is always established in between the reactant and the activated complex regardless of the relationship of the reactant and the product (if they are in equilibrium). This part of the theory can be materialised in the form of a mathematical expression through the Van Hoff equation. The equation describes an equilibrium state, which is reversible and temperature dependent. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{d\ln K}{dT} = \frac{\Delta U}{RT^{2}}&amp;lt;/math&amp;gt;    &#039;&#039;where, K - eq. constant, T - temperature in K, U - internal energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In order to get the temperature dependence of reaction rates, the equation is derived and as a result the Arrhenius equation is being formulated. The Arrhenius equation shows the temperature dependence of reaction rates as well as the activation energy of a corresponding reaction.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;k = Ae^{-E_a/RT}&amp;lt;/math&amp;gt;     &#039;&#039;where k - rate constant, T - temperature in K, A - exponential factor, Ea - activation energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
According to the theory, the last reaction -  where P1 and P2 were -2.5 and -5.0 respectively - must go to completion. However, the exact opposite was observed. As a conclusion, it is suggested that the rate constant is lower in real life than it is in theory. Therefore, the rate constant prevents the reaction from going to completion. (the energy barrier is sufficient to retain AB as a molecule when is it being subjected to a collision by C)&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This is sort of the right idea but a bit confused! Yes, TST states that once a reaction has reached the TS and crossed over to the product side, it will not cross back to the reactant side (the assumption of TST is the idea of no barrier recrossing). However in real life barrier recrossing can occur. Therefore the rate constant will be overpredicted by TST, as you have said. However, the rate constant does not prevent the reaction from going to completion and I cannot quite understand what you mean by this point. The main idea is there though. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:14, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;System of F-H-H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Classification of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:FH_E_surface.png]]&lt;br /&gt;
&lt;br /&gt;
Atoms A and B are H-s, whereas C was F. The surface plot (&#039;&#039;see above&#039;&#039;) shows that the reactants (on the right hand side) are higher in energy than the product (on the left hand side). Therefore the reaction:&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H &lt;br /&gt;
&lt;br /&gt;
is exothermic (negative sign, accompanied by a decrease in energy). Hence the reverse reaction: &lt;br /&gt;
&lt;br /&gt;
H + HF → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F&lt;br /&gt;
&lt;br /&gt;
must be endothermic, as this is the corresponding backward reaction. In that case, the reactants will be lower in energy and the products will be higher. Additional energy is required to pass the activation energy barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:HF_surfce_endothemic.png]] &lt;br /&gt;
&lt;br /&gt;
The first reaction is exothermic, (bond making is exothermic) which means that the final product will be in a lower energy state than the reactants. Hence, the HF bond is a stronger bond and is lower in energy than the H-H bond. This is due to the ionic nature of the H-F bond due to a large difference in electronegativity. The surface plot of the endothermic reaction is shown above. It can be depicted that the reactant are in a lower energy state than the product.&lt;br /&gt;
For these calculations p1=p2=0&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Really good answer. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:16, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Position of the Transition State&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_plot_norxn.png]]      [[File:Contour_norxn.png]]&lt;br /&gt;
&lt;br /&gt;
To find the transition state, the surface (above, on the left) and contour (above, on the right) plots were displayed. At a transition state, only a single black dot can been seen on a surface plot as there is no trajectory. Moreover, the contour plot was left blank, as the reaction did not happen, but no oscillation is observed as the vibrational freedom of the complex is being retained. The transition state was obtained at H-H distance: 0.745 Å, and H-F distance: 1.808 Å.&lt;br /&gt;
&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 Activation Energies &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Using the Energy vs Time plots, the following values have been established:&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F → HF + H:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -103.913 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 0.226 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -132.455 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 28.768 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|You should show the plots as it is not clear how these values were obtained. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:17, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Mechanisms of energy release&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
A scenario was set up in which the Animation and Momenta vs Time plots show that the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; - F reaction goes to completion. B and C were the H and A was the F atoms, with distances of A-B 1.5 Å, and B-C 0.878 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:mom_vs_time_AB_1.5_BC_0.878.png]]&lt;br /&gt;
&lt;br /&gt;
When the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule collides with the F atom, the translational energy of the species (due to the attraction between them) is being transformed into vibrational energy (oscillation being observed). Depending on the nature of the experiment, exothermic reactions release whereas, endothermic reactions absorb energy (in the form of heat) from the environment. When the oscillating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (both) atom approaches the  F atom (only translational energy), oscillation in the form of vibrational energy is being transmitted to the residual HF molecule. This way, the energy of the system is constant but the vibrational and kinetic energies are being transformed in between species. This can be confirmed experimentally by measuring the vibrational energy of the system via IR spectroscopy or use bomb calorimetry to determine the kinetic energy of the system  - which is directly proportional to the translational energy and its momentum. &lt;br /&gt;
&lt;br /&gt;
rHH = 0.74 Å, with a momentum pFH = -0.5, pHH in the range -3 to 3, rHF was set to 1.5 Å&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! pHH !! Level of Vibration of H-H bond !! Reaction &lt;br /&gt;
|-&lt;br /&gt;
| -3 || medium || transition state &lt;br /&gt;
|-&lt;br /&gt;
| -2.9 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.8 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.7 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.6 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.25 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
|  -2|| medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| -1 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 0 || strong|| yes &lt;br /&gt;
|-&lt;br /&gt;
| 1 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 1.5 || weak || transition state &lt;br /&gt;
|-&lt;br /&gt;
|  2 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.25  || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.3 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.4 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.6 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.7 ||  weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
|  2.8 || weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| 2.9  || weak || yes  &lt;br /&gt;
|-&lt;br /&gt;
| 3 || medium || yes &lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction goes to completion between the values -1.5 and 1, 2.5-2.6 and 2.9-3.0. As a conclusion, it was determined that no certain trends can be depicted from the data which would link the momentum, the outcome and the stretch of vibrations together. Moreover, the reactions at 2.9 and 3.0 are against Polanyi&#039;s empirical rule.&lt;br /&gt;
&lt;br /&gt;
For a separate calculation, the same initial positions were used, for HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F  with rHH=0.74 A but the momentum of HF was changed to p= -0.8 and the HH momentum was 0.1. The reaction goes to completion and thus the reaction is valid!&lt;br /&gt;
&lt;br /&gt;
If we look at the Momenta vs Time plot, we can see a continuously oscillating path, hence the reaction had reached its end. A large momentum contribution is seen as a a result of a large contribution from the very strong HF bond. &lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; 2 Å&lt;br /&gt;
HF 0.893325 Å&lt;br /&gt;
Phh - 8&lt;br /&gt;
Phf -0,02&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|It would be best to include figures in the table to show the trajectory being reactive/unreactive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:22, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5 Polanyi&#039;s Empirical Rule and the Distribution of Energy &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Polany&#039;s empirical rules&amp;lt;ref name=&amp;quot;No.2&amp;quot; /&amp;gt; are reflecting on the effect of transition states energetically different modes. An exothermic reaction - in which the products are higher in energy - the transition state is described as &#039;early&#039; as it is closer in energy to the reactants. Hence, the translational energy has a greater impact on the activated complex snd thus the reaction then the vibrational energy. Empirically, for an endothermic reaction -  with a corresponding late transition state - the vibrational energy has a greater importance on the reaction.&lt;br /&gt;
&lt;br /&gt;
In this case, &lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H&lt;br /&gt;
&lt;br /&gt;
is an exothermic reaction. Therefore, as described above it has an early transition state which suggest a greater impact from the translational energy contribution. The vibrational energy can be seen through the oscillating nature of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, where the translational contribution is largely coming from the H-F bond (both can be seen through their momenta). The effect of HH momentum is low. Therefore, larger HF contribution (momentum) would increase the chances of the reaction being completed. The experiment has failed to show a specific trend which would also comply with the theory. The results at 2.9 and 3 violate Polanyi&#039;s rules as discussed in the previous question. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.1&amp;quot;&amp;gt;T. Bligaard, J.K. Nørskov, in Chemical Bonding at Surfaces and Interfaces, 2008&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.2&amp;quot;&amp;gt;Polanyi, J. C. Concepts in Reaction Dynamics Acc. Chem. Res. 1972, 5, 161– 168&amp;lt;/ref&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793687</id>
		<title>MRD:MToth96</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793687"/>
		<updated>2019-05-28T11:17:43Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /*  Q3 Activation Energies  */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Collision of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Potential Energy Surface&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
 [[File:Surface_Plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface (&#039;&#039;see above&#039;&#039;), the transition state is found and defined as the point where it is true that ∂V(ri)/∂ri=0, and ∂V2(ri)/∂ri2&amp;gt;0.                       &lt;br /&gt;
Empirically, the gradient of the surface is hence equals zero. Looking at the surface plot, the kinetic energy surface, as a function of AB distance has &lt;br /&gt;
a curvature that describes the potential energy as a function of distance. The transition state is at its minimum, as the distances are in balance. &lt;br /&gt;
Also, the trajectory (see black line) has to have its maximum value at the transition state, as we are expecting an energy maximum at this point. &lt;br /&gt;
The transition state is the highest point along the trajectory. At this point, AB and BC are also equal. After the second differentiation, a local maximum &lt;br /&gt;
is found if the derived value is positive. It is distinguished from other local minima by implementing the following criterium: ∂V/dq1 = 0 and ∂V/dq2 = 0, &lt;br /&gt;
where q1 is the tangent to the minimum and q2 is orthogonal to this as well as to the reaction path. Hence, ∂V2/dq12 &amp;lt; 0 and ∂V2/dq22 &amp;gt; 0 for that point.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This isn&#039;t quite correct. The transition state is both a maximum and a minimum, in different directions. In the direction of the minimum energy trajectory (i.e. the path the black line follows) it is a maximum. The second partial derivative of a maximum is always negative. Therefore the second partial derivative of the function of the PES in the direction of the reaction trajectory will be negative. However, as the TS occurs on the minimum energy pathway, this point is also a minimum, but in a direction orthogonal to the reaction trajectory. Therefore, as the second partial derivative of a minimum is always positive, the second partial derivative of the PES at the TS in the direction orthogonal to the trajectory will be positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:04, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Locating Transition States&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
When the transition state is reached, both the AB and BC distances are equal. Atoms show no vibration and therefore the graph displays no straight lines in accordance with this observation. The optimal distance was found to be 0.908 Å, at which both AB and BC distances were equal. Also, the momentum for both p1 and p2 were set to zero. &lt;br /&gt;
The Intermolecular distanced vs Time plot is shown below (on the left). The aim was to minimise oscillation and obtain flat lines with no corresponding gradients. No vibration means no change in distance and the vibration of the H atom and molecule is restricted. A restriction in vibrational freedom means that the TS is reached. Moreover, the BC and AB distances are equal and the corresponding lines are on top of each other. A static picture of the animation of the transition state can be seen below (on the right)&lt;br /&gt;
&lt;br /&gt;
[[File:Diastance_vs_time_h2.PNG]] .     [[File:Animation_h2_static.PNG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Why does a restriction in vibrational freedom mean that the TS is reached? Also be careful - the distance AB=BC at the TS only for a symmetrical reaction and that is only because reactants = products. This is not true of any TS. Perhaps you are aware of this, but you need to state it explicitly in order for this statement to be true. I also do not understand your point stating that &amp;quot;the graph displays no straight lines&amp;quot; where there is no vibration. What straight lines? In order to be very clear about what you mean, you need to explain every point you make thoroughly.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:07, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 MEP and Dynamic Trajectory&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_mep.PNG]] .     [[File:Surface_dynamic.PNG]]&lt;br /&gt;
&lt;br /&gt;
The trajectory is displayed as the black line along the bottom of the surface plots (&#039;&#039;see above&#039;&#039;. When the MEP calculation (on the left) is used, the line starts from the transition state but is only displayed for a short length. Whereas, the dynamic calculation (on the right) gives a much longer, complete black trajectory. The program tries to find the steepest descent along the potential energy surface to obtained a minimum. The MEP method is being reset to zero after every step, whilst with dynamic calculation the data is being carried further to the next step. Hence, the calculation is being carried on regardless, whereas with MEP the kinetic energy stays at its minimum. Thus, an oscillating line with the dynamic, and a local maximum with the MEP calculation is being observed. &lt;br /&gt;
&lt;br /&gt;
[[File:normal.PNG]]               [[File:Changed_distance.PNG]]&lt;br /&gt;
&lt;br /&gt;
For comparison, values of interatomic distances were changed (&#039;&#039;see above&#039;&#039;. Values were being shifted from r1=ts+0.01, r2=ts (on the left); to r1=ts and r2=ts+0.01 (on the right)&lt;br /&gt;
In both cases, it was observed that the lines corresponding to the AB and BC distances were exchanged (as expected). When the numbers got changed, the transition state was approached by the opposite direction - as a symmetrical system is being considered - and the values are exactly the same but opposite. Hence, the same plot was displayed in the opposite direction. The same variations were applied for Momenta vs Time plots. The observations are exactly the same as for the distances, with the position of the lines being exchanged in between. The initial values are displayed below on the left, whereas the changed values can be seen on the right.&lt;br /&gt;
&lt;br /&gt;
[[File:Normal_momentum.PNG]]         [[File:Changed.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Reactivity through trajectory analysis &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; (kcal.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;
| -1.25 || -2.5  || -99.018 || Yes || A-B oscillates, B and C bond formation || [[File:-1.25,-2.5_p1,p2.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  || -100.456 || No || A-B oscillates, no reaction || [[File:-1.5,-2.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  || -98.956 || Yes || A-B oscillates, B and C bond formation || [[File:-1.5,-2.5.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  || -84.956 || No ||  A-B oscillates intensely, B and C bond formation is expected, but it bounces off and C remains a single atom || [[File:-2.5,-5.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  || -83.416 || Yes || 	A-B oscillates intensely, very close transition state, B and C bond formation || [[File:-2.5,-5.2.png]]&lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
From the table above it was concluded that the E total of the system depends on the momentum. Moreover, it shows a correlation with the kinetic energy of the system. The potential energy is constant and the kinetic energy is changing in response the structural changes. Furthermore, the system&#039;s susceptibility to undergo a reaction is also dependent on the momentum (not just on energy). If there is a large momentum difference between the single atom and the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule - especially when the incoming atom&#039;s momentum is marginally lower - than the reaction will not happen.&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5  Transition State Theory &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Transition State theory&amp;lt;ref name=&amp;quot;No.1&amp;quot; /&amp;gt; is a way of describing chemical reactions as such that the reaction consist of atoms and molecules are subjected to a continuous change in the energies and positions. The transition state is being described as the position along the reaction path where the energy is at its maximum. The activation energy corresponding to a specific reaction and to its reactant is the energy necessary to initiate collisions sufficient to reach the transition state. It is calculated as the difference between the reactants and the transition state. The transition state or activated complex is in equilibrium with the reactant and hence its properties can be approximated using Hammond&#039;s postulate. Moreover, the rate if reaction - formation of products - can be approximates from the concentration of these activated complexes and their ability to go to completion.&lt;br /&gt;
&lt;br /&gt;
Furthermore, the transition state theory can also be applied to the quasi-equilibrium state. The reactants are in equilibrium with the transition state complex. This means that an equilibrium is always established in between the reactant and the activated complex regardless of the relationship of the reactant and the product (if they are in equilibrium). This part of the theory can be materialised in the form of a mathematical expression through the Van Hoff equation. The equation describes an equilibrium state, which is reversible and temperature dependent. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{d\ln K}{dT} = \frac{\Delta U}{RT^{2}}&amp;lt;/math&amp;gt;    &#039;&#039;where, K - eq. constant, T - temperature in K, U - internal energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In order to get the temperature dependence of reaction rates, the equation is derived and as a result the Arrhenius equation is being formulated. The Arrhenius equation shows the temperature dependence of reaction rates as well as the activation energy of a corresponding reaction.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;k = Ae^{-E_a/RT}&amp;lt;/math&amp;gt;     &#039;&#039;where k - rate constant, T - temperature in K, A - exponential factor, Ea - activation energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
According to the theory, the last reaction -  where P1 and P2 were -2.5 and -5.0 respectively - must go to completion. However, the exact opposite was observed. As a conclusion, it is suggested that the rate constant is lower in real life than it is in theory. Therefore, the rate constant prevents the reaction from going to completion. (the energy barrier is sufficient to retain AB as a molecule when is it being subjected to a collision by C)&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This is sort of the right idea but a bit confused! Yes, TST states that once a reaction has reached the TS and crossed over to the product side, it will not cross back to the reactant side (the assumption of TST is the idea of no barrier recrossing). However in real life barrier recrossing can occur. Therefore the rate constant will be overpredicted by TST, as you have said. However, the rate constant does not prevent the reaction from going to completion and I cannot quite understand what you mean by this point. The main idea is there though. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:14, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;System of F-H-H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Classification of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:FH_E_surface.png]]&lt;br /&gt;
&lt;br /&gt;
Atoms A and B are H-s, whereas C was F. The surface plot (&#039;&#039;see above&#039;&#039;) shows that the reactants (on the right hand side) are higher in energy than the product (on the left hand side). Therefore the reaction:&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H &lt;br /&gt;
&lt;br /&gt;
is exothermic (negative sign, accompanied by a decrease in energy). Hence the reverse reaction: &lt;br /&gt;
&lt;br /&gt;
H + HF → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F&lt;br /&gt;
&lt;br /&gt;
must be endothermic, as this is the corresponding backward reaction. In that case, the reactants will be lower in energy and the products will be higher. Additional energy is required to pass the activation energy barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:HF_surfce_endothemic.png]] &lt;br /&gt;
&lt;br /&gt;
The first reaction is exothermic, (bond making is exothermic) which means that the final product will be in a lower energy state than the reactants. Hence, the HF bond is a stronger bond and is lower in energy than the H-H bond. This is due to the ionic nature of the H-F bond due to a large difference in electronegativity. The surface plot of the endothermic reaction is shown above. It can be depicted that the reactant are in a lower energy state than the product.&lt;br /&gt;
For these calculations p1=p2=0&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Really good answer. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:16, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Position of the Transition State&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_plot_norxn.png]]      [[File:Contour_norxn.png]]&lt;br /&gt;
&lt;br /&gt;
To find the transition state, the surface (above, on the left) and contour (above, on the right) plots were displayed. At a transition state, only a single black dot can been seen on a surface plot as there is no trajectory. Moreover, the contour plot was left blank, as the reaction did not happen, but no oscillation is observed as the vibrational freedom of the complex is being retained. The transition state was obtained at H-H distance: 0.745 Å, and H-F distance: 1.808 Å.&lt;br /&gt;
&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 Activation Energies &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Using the Energy vs Time plots, the following values have been established:&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F → HF + H:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -103.913 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 0.226 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -132.455 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 28.768 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|You should show the plots as it is not clear how these values were obtained. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:17, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Mechanisms of energy release&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
A scenario was set up in which the Animation and Momenta vs Time plots show that the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; - F reaction goes to completion. B and C were the H and A was the F atoms, with distances of A-B 1.5 Å, and B-C 0.878 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:mom_vs_time_AB_1.5_BC_0.878.png]]&lt;br /&gt;
&lt;br /&gt;
When the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule collides with the F atom, the translational energy of the species (due to the attraction between them) is being transformed into vibrational energy (oscillation being observed). Depending on the nature of the experiment, exothermic reactions release whereas, endothermic reactions absorb energy (in the form of heat) from the environment. When the oscillating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (both) atom approaches the  F atom (only translational energy), oscillation in the form of vibrational energy is being transmitted to the residual HF molecule. This way, the energy of the system is constant but the vibrational and kinetic energies are being transformed in between species. This can be confirmed experimentally by measuring the vibrational energy of the system via IR spectroscopy or use bomb calorimetry to determine the kinetic energy of the system  - which is directly proportional to the translational energy and its momentum. &lt;br /&gt;
&lt;br /&gt;
rHH = 0.74 Å, with a momentum pFH = -0.5, pHH in the range -3 to 3, rHF was set to 1.5 Å&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! pHH !! Level of Vibration of H-H bond !! Reaction &lt;br /&gt;
|-&lt;br /&gt;
| -3 || medium || transition state &lt;br /&gt;
|-&lt;br /&gt;
| -2.9 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.8 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.7 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.6 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.25 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
|  -2|| medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| -1 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 0 || strong|| yes &lt;br /&gt;
|-&lt;br /&gt;
| 1 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 1.5 || weak || transition state &lt;br /&gt;
|-&lt;br /&gt;
|  2 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.25  || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.3 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.4 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.6 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.7 ||  weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
|  2.8 || weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| 2.9  || weak || yes  &lt;br /&gt;
|-&lt;br /&gt;
| 3 || medium || yes &lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction goes to completion between the values -1.5 and 1, 2.5-2.6 and 2.9-3.0. As a conclusion, it was determined that no certain trends can be depicted from the data which would link the momentum, the outcome and the stretch of vibrations together. Moreover, the reactions at 2.9 and 3.0 are against Polanyi&#039;s empirical rule.&lt;br /&gt;
&lt;br /&gt;
For a separate calculation, the same initial positions were used, for HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F  with rHH=0.74 A but the momentum of HF was changed to p= -0.8 and the HH momentum was 0.1. The reaction goes to completion and thus the reaction is valid!&lt;br /&gt;
&lt;br /&gt;
If we look at the Momenta vs Time plot, we can see a continuously oscillating path, hence the reaction had reached its end. A large momentum contribution is seen as a a result of a large contribution from the very strong HF bond. &lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; 2 Å&lt;br /&gt;
HF 0.893325 Å&lt;br /&gt;
Phh - 8&lt;br /&gt;
Phf -0,02&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5 Polanyi&#039;s Empirical Rule and the Distribution of Energy &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Polany&#039;s empirical rules&amp;lt;ref name=&amp;quot;No.2&amp;quot; /&amp;gt; are reflecting on the effect of transition states energetically different modes. An exothermic reaction - in which the products are higher in energy - the transition state is described as &#039;early&#039; as it is closer in energy to the reactants. Hence, the translational energy has a greater impact on the activated complex snd thus the reaction then the vibrational energy. Empirically, for an endothermic reaction -  with a corresponding late transition state - the vibrational energy has a greater importance on the reaction.&lt;br /&gt;
&lt;br /&gt;
In this case, &lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H&lt;br /&gt;
&lt;br /&gt;
is an exothermic reaction. Therefore, as described above it has an early transition state which suggest a greater impact from the translational energy contribution. The vibrational energy can be seen through the oscillating nature of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, where the translational contribution is largely coming from the H-F bond (both can be seen through their momenta). The effect of HH momentum is low. Therefore, larger HF contribution (momentum) would increase the chances of the reaction being completed. The experiment has failed to show a specific trend which would also comply with the theory. The results at 2.9 and 3 violate Polanyi&#039;s rules as discussed in the previous question. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.1&amp;quot;&amp;gt;T. Bligaard, J.K. Nørskov, in Chemical Bonding at Surfaces and Interfaces, 2008&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.2&amp;quot;&amp;gt;Polanyi, J. C. Concepts in Reaction Dynamics Acc. Chem. Res. 1972, 5, 161– 168&amp;lt;/ref&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793686</id>
		<title>MRD:MToth96</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793686"/>
		<updated>2019-05-28T11:16:14Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /*  Q1 Classification of F + H2 and H + HF reactions  */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Collision of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Potential Energy Surface&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
 [[File:Surface_Plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface (&#039;&#039;see above&#039;&#039;), the transition state is found and defined as the point where it is true that ∂V(ri)/∂ri=0, and ∂V2(ri)/∂ri2&amp;gt;0.                       &lt;br /&gt;
Empirically, the gradient of the surface is hence equals zero. Looking at the surface plot, the kinetic energy surface, as a function of AB distance has &lt;br /&gt;
a curvature that describes the potential energy as a function of distance. The transition state is at its minimum, as the distances are in balance. &lt;br /&gt;
Also, the trajectory (see black line) has to have its maximum value at the transition state, as we are expecting an energy maximum at this point. &lt;br /&gt;
The transition state is the highest point along the trajectory. At this point, AB and BC are also equal. After the second differentiation, a local maximum &lt;br /&gt;
is found if the derived value is positive. It is distinguished from other local minima by implementing the following criterium: ∂V/dq1 = 0 and ∂V/dq2 = 0, &lt;br /&gt;
where q1 is the tangent to the minimum and q2 is orthogonal to this as well as to the reaction path. Hence, ∂V2/dq12 &amp;lt; 0 and ∂V2/dq22 &amp;gt; 0 for that point.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This isn&#039;t quite correct. The transition state is both a maximum and a minimum, in different directions. In the direction of the minimum energy trajectory (i.e. the path the black line follows) it is a maximum. The second partial derivative of a maximum is always negative. Therefore the second partial derivative of the function of the PES in the direction of the reaction trajectory will be negative. However, as the TS occurs on the minimum energy pathway, this point is also a minimum, but in a direction orthogonal to the reaction trajectory. Therefore, as the second partial derivative of a minimum is always positive, the second partial derivative of the PES at the TS in the direction orthogonal to the trajectory will be positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:04, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Locating Transition States&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
When the transition state is reached, both the AB and BC distances are equal. Atoms show no vibration and therefore the graph displays no straight lines in accordance with this observation. The optimal distance was found to be 0.908 Å, at which both AB and BC distances were equal. Also, the momentum for both p1 and p2 were set to zero. &lt;br /&gt;
The Intermolecular distanced vs Time plot is shown below (on the left). The aim was to minimise oscillation and obtain flat lines with no corresponding gradients. No vibration means no change in distance and the vibration of the H atom and molecule is restricted. A restriction in vibrational freedom means that the TS is reached. Moreover, the BC and AB distances are equal and the corresponding lines are on top of each other. A static picture of the animation of the transition state can be seen below (on the right)&lt;br /&gt;
&lt;br /&gt;
[[File:Diastance_vs_time_h2.PNG]] .     [[File:Animation_h2_static.PNG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Why does a restriction in vibrational freedom mean that the TS is reached? Also be careful - the distance AB=BC at the TS only for a symmetrical reaction and that is only because reactants = products. This is not true of any TS. Perhaps you are aware of this, but you need to state it explicitly in order for this statement to be true. I also do not understand your point stating that &amp;quot;the graph displays no straight lines&amp;quot; where there is no vibration. What straight lines? In order to be very clear about what you mean, you need to explain every point you make thoroughly.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:07, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 MEP and Dynamic Trajectory&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_mep.PNG]] .     [[File:Surface_dynamic.PNG]]&lt;br /&gt;
&lt;br /&gt;
The trajectory is displayed as the black line along the bottom of the surface plots (&#039;&#039;see above&#039;&#039;. When the MEP calculation (on the left) is used, the line starts from the transition state but is only displayed for a short length. Whereas, the dynamic calculation (on the right) gives a much longer, complete black trajectory. The program tries to find the steepest descent along the potential energy surface to obtained a minimum. The MEP method is being reset to zero after every step, whilst with dynamic calculation the data is being carried further to the next step. Hence, the calculation is being carried on regardless, whereas with MEP the kinetic energy stays at its minimum. Thus, an oscillating line with the dynamic, and a local maximum with the MEP calculation is being observed. &lt;br /&gt;
&lt;br /&gt;
[[File:normal.PNG]]               [[File:Changed_distance.PNG]]&lt;br /&gt;
&lt;br /&gt;
For comparison, values of interatomic distances were changed (&#039;&#039;see above&#039;&#039;. Values were being shifted from r1=ts+0.01, r2=ts (on the left); to r1=ts and r2=ts+0.01 (on the right)&lt;br /&gt;
In both cases, it was observed that the lines corresponding to the AB and BC distances were exchanged (as expected). When the numbers got changed, the transition state was approached by the opposite direction - as a symmetrical system is being considered - and the values are exactly the same but opposite. Hence, the same plot was displayed in the opposite direction. The same variations were applied for Momenta vs Time plots. The observations are exactly the same as for the distances, with the position of the lines being exchanged in between. The initial values are displayed below on the left, whereas the changed values can be seen on the right.&lt;br /&gt;
&lt;br /&gt;
[[File:Normal_momentum.PNG]]         [[File:Changed.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Reactivity through trajectory analysis &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; (kcal.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;
| -1.25 || -2.5  || -99.018 || Yes || A-B oscillates, B and C bond formation || [[File:-1.25,-2.5_p1,p2.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  || -100.456 || No || A-B oscillates, no reaction || [[File:-1.5,-2.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  || -98.956 || Yes || A-B oscillates, B and C bond formation || [[File:-1.5,-2.5.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  || -84.956 || No ||  A-B oscillates intensely, B and C bond formation is expected, but it bounces off and C remains a single atom || [[File:-2.5,-5.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  || -83.416 || Yes || 	A-B oscillates intensely, very close transition state, B and C bond formation || [[File:-2.5,-5.2.png]]&lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
From the table above it was concluded that the E total of the system depends on the momentum. Moreover, it shows a correlation with the kinetic energy of the system. The potential energy is constant and the kinetic energy is changing in response the structural changes. Furthermore, the system&#039;s susceptibility to undergo a reaction is also dependent on the momentum (not just on energy). If there is a large momentum difference between the single atom and the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule - especially when the incoming atom&#039;s momentum is marginally lower - than the reaction will not happen.&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5  Transition State Theory &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Transition State theory&amp;lt;ref name=&amp;quot;No.1&amp;quot; /&amp;gt; is a way of describing chemical reactions as such that the reaction consist of atoms and molecules are subjected to a continuous change in the energies and positions. The transition state is being described as the position along the reaction path where the energy is at its maximum. The activation energy corresponding to a specific reaction and to its reactant is the energy necessary to initiate collisions sufficient to reach the transition state. It is calculated as the difference between the reactants and the transition state. The transition state or activated complex is in equilibrium with the reactant and hence its properties can be approximated using Hammond&#039;s postulate. Moreover, the rate if reaction - formation of products - can be approximates from the concentration of these activated complexes and their ability to go to completion.&lt;br /&gt;
&lt;br /&gt;
Furthermore, the transition state theory can also be applied to the quasi-equilibrium state. The reactants are in equilibrium with the transition state complex. This means that an equilibrium is always established in between the reactant and the activated complex regardless of the relationship of the reactant and the product (if they are in equilibrium). This part of the theory can be materialised in the form of a mathematical expression through the Van Hoff equation. The equation describes an equilibrium state, which is reversible and temperature dependent. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{d\ln K}{dT} = \frac{\Delta U}{RT^{2}}&amp;lt;/math&amp;gt;    &#039;&#039;where, K - eq. constant, T - temperature in K, U - internal energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In order to get the temperature dependence of reaction rates, the equation is derived and as a result the Arrhenius equation is being formulated. The Arrhenius equation shows the temperature dependence of reaction rates as well as the activation energy of a corresponding reaction.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;k = Ae^{-E_a/RT}&amp;lt;/math&amp;gt;     &#039;&#039;where k - rate constant, T - temperature in K, A - exponential factor, Ea - activation energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
According to the theory, the last reaction -  where P1 and P2 were -2.5 and -5.0 respectively - must go to completion. However, the exact opposite was observed. As a conclusion, it is suggested that the rate constant is lower in real life than it is in theory. Therefore, the rate constant prevents the reaction from going to completion. (the energy barrier is sufficient to retain AB as a molecule when is it being subjected to a collision by C)&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This is sort of the right idea but a bit confused! Yes, TST states that once a reaction has reached the TS and crossed over to the product side, it will not cross back to the reactant side (the assumption of TST is the idea of no barrier recrossing). However in real life barrier recrossing can occur. Therefore the rate constant will be overpredicted by TST, as you have said. However, the rate constant does not prevent the reaction from going to completion and I cannot quite understand what you mean by this point. The main idea is there though. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:14, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;System of F-H-H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Classification of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:FH_E_surface.png]]&lt;br /&gt;
&lt;br /&gt;
Atoms A and B are H-s, whereas C was F. The surface plot (&#039;&#039;see above&#039;&#039;) shows that the reactants (on the right hand side) are higher in energy than the product (on the left hand side). Therefore the reaction:&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H &lt;br /&gt;
&lt;br /&gt;
is exothermic (negative sign, accompanied by a decrease in energy). Hence the reverse reaction: &lt;br /&gt;
&lt;br /&gt;
H + HF → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F&lt;br /&gt;
&lt;br /&gt;
must be endothermic, as this is the corresponding backward reaction. In that case, the reactants will be lower in energy and the products will be higher. Additional energy is required to pass the activation energy barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:HF_surfce_endothemic.png]] &lt;br /&gt;
&lt;br /&gt;
The first reaction is exothermic, (bond making is exothermic) which means that the final product will be in a lower energy state than the reactants. Hence, the HF bond is a stronger bond and is lower in energy than the H-H bond. This is due to the ionic nature of the H-F bond due to a large difference in electronegativity. The surface plot of the endothermic reaction is shown above. It can be depicted that the reactant are in a lower energy state than the product.&lt;br /&gt;
For these calculations p1=p2=0&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Really good answer. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:16, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Position of the Transition State&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_plot_norxn.png]]      [[File:Contour_norxn.png]]&lt;br /&gt;
&lt;br /&gt;
To find the transition state, the surface (above, on the left) and contour (above, on the right) plots were displayed. At a transition state, only a single black dot can been seen on a surface plot as there is no trajectory. Moreover, the contour plot was left blank, as the reaction did not happen, but no oscillation is observed as the vibrational freedom of the complex is being retained. The transition state was obtained at H-H distance: 0.745 Å, and H-F distance: 1.808 Å.&lt;br /&gt;
&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 Activation Energies &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Using the Energy vs Time plots, the following values have been established:&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F → HF + H:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -103.913 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 0.226 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -132.455 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 28.768 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Mechanisms of energy release&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
A scenario was set up in which the Animation and Momenta vs Time plots show that the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; - F reaction goes to completion. B and C were the H and A was the F atoms, with distances of A-B 1.5 Å, and B-C 0.878 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:mom_vs_time_AB_1.5_BC_0.878.png]]&lt;br /&gt;
&lt;br /&gt;
When the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule collides with the F atom, the translational energy of the species (due to the attraction between them) is being transformed into vibrational energy (oscillation being observed). Depending on the nature of the experiment, exothermic reactions release whereas, endothermic reactions absorb energy (in the form of heat) from the environment. When the oscillating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (both) atom approaches the  F atom (only translational energy), oscillation in the form of vibrational energy is being transmitted to the residual HF molecule. This way, the energy of the system is constant but the vibrational and kinetic energies are being transformed in between species. This can be confirmed experimentally by measuring the vibrational energy of the system via IR spectroscopy or use bomb calorimetry to determine the kinetic energy of the system  - which is directly proportional to the translational energy and its momentum. &lt;br /&gt;
&lt;br /&gt;
rHH = 0.74 Å, with a momentum pFH = -0.5, pHH in the range -3 to 3, rHF was set to 1.5 Å&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! pHH !! Level of Vibration of H-H bond !! Reaction &lt;br /&gt;
|-&lt;br /&gt;
| -3 || medium || transition state &lt;br /&gt;
|-&lt;br /&gt;
| -2.9 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.8 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.7 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.6 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.25 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
|  -2|| medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| -1 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 0 || strong|| yes &lt;br /&gt;
|-&lt;br /&gt;
| 1 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 1.5 || weak || transition state &lt;br /&gt;
|-&lt;br /&gt;
|  2 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.25  || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.3 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.4 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.6 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.7 ||  weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
|  2.8 || weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| 2.9  || weak || yes  &lt;br /&gt;
|-&lt;br /&gt;
| 3 || medium || yes &lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction goes to completion between the values -1.5 and 1, 2.5-2.6 and 2.9-3.0. As a conclusion, it was determined that no certain trends can be depicted from the data which would link the momentum, the outcome and the stretch of vibrations together. Moreover, the reactions at 2.9 and 3.0 are against Polanyi&#039;s empirical rule.&lt;br /&gt;
&lt;br /&gt;
For a separate calculation, the same initial positions were used, for HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F  with rHH=0.74 A but the momentum of HF was changed to p= -0.8 and the HH momentum was 0.1. The reaction goes to completion and thus the reaction is valid!&lt;br /&gt;
&lt;br /&gt;
If we look at the Momenta vs Time plot, we can see a continuously oscillating path, hence the reaction had reached its end. A large momentum contribution is seen as a a result of a large contribution from the very strong HF bond. &lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; 2 Å&lt;br /&gt;
HF 0.893325 Å&lt;br /&gt;
Phh - 8&lt;br /&gt;
Phf -0,02&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5 Polanyi&#039;s Empirical Rule and the Distribution of Energy &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Polany&#039;s empirical rules&amp;lt;ref name=&amp;quot;No.2&amp;quot; /&amp;gt; are reflecting on the effect of transition states energetically different modes. An exothermic reaction - in which the products are higher in energy - the transition state is described as &#039;early&#039; as it is closer in energy to the reactants. Hence, the translational energy has a greater impact on the activated complex snd thus the reaction then the vibrational energy. Empirically, for an endothermic reaction -  with a corresponding late transition state - the vibrational energy has a greater importance on the reaction.&lt;br /&gt;
&lt;br /&gt;
In this case, &lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H&lt;br /&gt;
&lt;br /&gt;
is an exothermic reaction. Therefore, as described above it has an early transition state which suggest a greater impact from the translational energy contribution. The vibrational energy can be seen through the oscillating nature of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, where the translational contribution is largely coming from the H-F bond (both can be seen through their momenta). The effect of HH momentum is low. Therefore, larger HF contribution (momentum) would increase the chances of the reaction being completed. The experiment has failed to show a specific trend which would also comply with the theory. The results at 2.9 and 3 violate Polanyi&#039;s rules as discussed in the previous question. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.1&amp;quot;&amp;gt;T. Bligaard, J.K. Nørskov, in Chemical Bonding at Surfaces and Interfaces, 2008&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.2&amp;quot;&amp;gt;Polanyi, J. C. Concepts in Reaction Dynamics Acc. Chem. Res. 1972, 5, 161– 168&amp;lt;/ref&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793685</id>
		<title>MRD:MToth96</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793685"/>
		<updated>2019-05-28T11:14:57Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /*  Q5  Transition State Theory  */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Collision of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Potential Energy Surface&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
 [[File:Surface_Plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface (&#039;&#039;see above&#039;&#039;), the transition state is found and defined as the point where it is true that ∂V(ri)/∂ri=0, and ∂V2(ri)/∂ri2&amp;gt;0.                       &lt;br /&gt;
Empirically, the gradient of the surface is hence equals zero. Looking at the surface plot, the kinetic energy surface, as a function of AB distance has &lt;br /&gt;
a curvature that describes the potential energy as a function of distance. The transition state is at its minimum, as the distances are in balance. &lt;br /&gt;
Also, the trajectory (see black line) has to have its maximum value at the transition state, as we are expecting an energy maximum at this point. &lt;br /&gt;
The transition state is the highest point along the trajectory. At this point, AB and BC are also equal. After the second differentiation, a local maximum &lt;br /&gt;
is found if the derived value is positive. It is distinguished from other local minima by implementing the following criterium: ∂V/dq1 = 0 and ∂V/dq2 = 0, &lt;br /&gt;
where q1 is the tangent to the minimum and q2 is orthogonal to this as well as to the reaction path. Hence, ∂V2/dq12 &amp;lt; 0 and ∂V2/dq22 &amp;gt; 0 for that point.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This isn&#039;t quite correct. The transition state is both a maximum and a minimum, in different directions. In the direction of the minimum energy trajectory (i.e. the path the black line follows) it is a maximum. The second partial derivative of a maximum is always negative. Therefore the second partial derivative of the function of the PES in the direction of the reaction trajectory will be negative. However, as the TS occurs on the minimum energy pathway, this point is also a minimum, but in a direction orthogonal to the reaction trajectory. Therefore, as the second partial derivative of a minimum is always positive, the second partial derivative of the PES at the TS in the direction orthogonal to the trajectory will be positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:04, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Locating Transition States&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
When the transition state is reached, both the AB and BC distances are equal. Atoms show no vibration and therefore the graph displays no straight lines in accordance with this observation. The optimal distance was found to be 0.908 Å, at which both AB and BC distances were equal. Also, the momentum for both p1 and p2 were set to zero. &lt;br /&gt;
The Intermolecular distanced vs Time plot is shown below (on the left). The aim was to minimise oscillation and obtain flat lines with no corresponding gradients. No vibration means no change in distance and the vibration of the H atom and molecule is restricted. A restriction in vibrational freedom means that the TS is reached. Moreover, the BC and AB distances are equal and the corresponding lines are on top of each other. A static picture of the animation of the transition state can be seen below (on the right)&lt;br /&gt;
&lt;br /&gt;
[[File:Diastance_vs_time_h2.PNG]] .     [[File:Animation_h2_static.PNG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Why does a restriction in vibrational freedom mean that the TS is reached? Also be careful - the distance AB=BC at the TS only for a symmetrical reaction and that is only because reactants = products. This is not true of any TS. Perhaps you are aware of this, but you need to state it explicitly in order for this statement to be true. I also do not understand your point stating that &amp;quot;the graph displays no straight lines&amp;quot; where there is no vibration. What straight lines? In order to be very clear about what you mean, you need to explain every point you make thoroughly.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:07, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 MEP and Dynamic Trajectory&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_mep.PNG]] .     [[File:Surface_dynamic.PNG]]&lt;br /&gt;
&lt;br /&gt;
The trajectory is displayed as the black line along the bottom of the surface plots (&#039;&#039;see above&#039;&#039;. When the MEP calculation (on the left) is used, the line starts from the transition state but is only displayed for a short length. Whereas, the dynamic calculation (on the right) gives a much longer, complete black trajectory. The program tries to find the steepest descent along the potential energy surface to obtained a minimum. The MEP method is being reset to zero after every step, whilst with dynamic calculation the data is being carried further to the next step. Hence, the calculation is being carried on regardless, whereas with MEP the kinetic energy stays at its minimum. Thus, an oscillating line with the dynamic, and a local maximum with the MEP calculation is being observed. &lt;br /&gt;
&lt;br /&gt;
[[File:normal.PNG]]               [[File:Changed_distance.PNG]]&lt;br /&gt;
&lt;br /&gt;
For comparison, values of interatomic distances were changed (&#039;&#039;see above&#039;&#039;. Values were being shifted from r1=ts+0.01, r2=ts (on the left); to r1=ts and r2=ts+0.01 (on the right)&lt;br /&gt;
In both cases, it was observed that the lines corresponding to the AB and BC distances were exchanged (as expected). When the numbers got changed, the transition state was approached by the opposite direction - as a symmetrical system is being considered - and the values are exactly the same but opposite. Hence, the same plot was displayed in the opposite direction. The same variations were applied for Momenta vs Time plots. The observations are exactly the same as for the distances, with the position of the lines being exchanged in between. The initial values are displayed below on the left, whereas the changed values can be seen on the right.&lt;br /&gt;
&lt;br /&gt;
[[File:Normal_momentum.PNG]]         [[File:Changed.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Reactivity through trajectory analysis &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; (kcal.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;
| -1.25 || -2.5  || -99.018 || Yes || A-B oscillates, B and C bond formation || [[File:-1.25,-2.5_p1,p2.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  || -100.456 || No || A-B oscillates, no reaction || [[File:-1.5,-2.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  || -98.956 || Yes || A-B oscillates, B and C bond formation || [[File:-1.5,-2.5.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  || -84.956 || No ||  A-B oscillates intensely, B and C bond formation is expected, but it bounces off and C remains a single atom || [[File:-2.5,-5.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  || -83.416 || Yes || 	A-B oscillates intensely, very close transition state, B and C bond formation || [[File:-2.5,-5.2.png]]&lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
From the table above it was concluded that the E total of the system depends on the momentum. Moreover, it shows a correlation with the kinetic energy of the system. The potential energy is constant and the kinetic energy is changing in response the structural changes. Furthermore, the system&#039;s susceptibility to undergo a reaction is also dependent on the momentum (not just on energy). If there is a large momentum difference between the single atom and the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule - especially when the incoming atom&#039;s momentum is marginally lower - than the reaction will not happen.&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5  Transition State Theory &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Transition State theory&amp;lt;ref name=&amp;quot;No.1&amp;quot; /&amp;gt; is a way of describing chemical reactions as such that the reaction consist of atoms and molecules are subjected to a continuous change in the energies and positions. The transition state is being described as the position along the reaction path where the energy is at its maximum. The activation energy corresponding to a specific reaction and to its reactant is the energy necessary to initiate collisions sufficient to reach the transition state. It is calculated as the difference between the reactants and the transition state. The transition state or activated complex is in equilibrium with the reactant and hence its properties can be approximated using Hammond&#039;s postulate. Moreover, the rate if reaction - formation of products - can be approximates from the concentration of these activated complexes and their ability to go to completion.&lt;br /&gt;
&lt;br /&gt;
Furthermore, the transition state theory can also be applied to the quasi-equilibrium state. The reactants are in equilibrium with the transition state complex. This means that an equilibrium is always established in between the reactant and the activated complex regardless of the relationship of the reactant and the product (if they are in equilibrium). This part of the theory can be materialised in the form of a mathematical expression through the Van Hoff equation. The equation describes an equilibrium state, which is reversible and temperature dependent. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{d\ln K}{dT} = \frac{\Delta U}{RT^{2}}&amp;lt;/math&amp;gt;    &#039;&#039;where, K - eq. constant, T - temperature in K, U - internal energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In order to get the temperature dependence of reaction rates, the equation is derived and as a result the Arrhenius equation is being formulated. The Arrhenius equation shows the temperature dependence of reaction rates as well as the activation energy of a corresponding reaction.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;k = Ae^{-E_a/RT}&amp;lt;/math&amp;gt;     &#039;&#039;where k - rate constant, T - temperature in K, A - exponential factor, Ea - activation energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
According to the theory, the last reaction -  where P1 and P2 were -2.5 and -5.0 respectively - must go to completion. However, the exact opposite was observed. As a conclusion, it is suggested that the rate constant is lower in real life than it is in theory. Therefore, the rate constant prevents the reaction from going to completion. (the energy barrier is sufficient to retain AB as a molecule when is it being subjected to a collision by C)&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This is sort of the right idea but a bit confused! Yes, TST states that once a reaction has reached the TS and crossed over to the product side, it will not cross back to the reactant side (the assumption of TST is the idea of no barrier recrossing). However in real life barrier recrossing can occur. Therefore the rate constant will be overpredicted by TST, as you have said. However, the rate constant does not prevent the reaction from going to completion and I cannot quite understand what you mean by this point. The main idea is there though. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:14, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;System of F-H-H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Classification of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:FH_E_surface.png]]&lt;br /&gt;
&lt;br /&gt;
Atoms A and B are H-s, whereas C was F. The surface plot (&#039;&#039;see above&#039;&#039;) shows that the reactants (on the right hand side) are higher in energy than the product (on the left hand side). Therefore the reaction:&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H &lt;br /&gt;
&lt;br /&gt;
is exothermic (negative sign, accompanied by a decrease in energy). Hence the reverse reaction: &lt;br /&gt;
&lt;br /&gt;
H + HF → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F&lt;br /&gt;
&lt;br /&gt;
must be endothermic, as this is the corresponding backward reaction. In that case, the reactants will be lower in energy and the products will be higher. Additional energy is required to pass the activation energy barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:HF_surfce_endothemic.png]] &lt;br /&gt;
&lt;br /&gt;
The first reaction is exothermic, (bond making is exothermic) which means that the final product will be in a lower energy state than the reactants. Hence, the HF bond is a stronger bond and is lower in energy than the H-H bond. This is due to the ionic nature of the H-F bond due to a large difference in electronegativity. The surface plot of the endothermic reaction is shown above. It can be depicted that the reactant are in a lower energy state than the product.&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Position of the Transition State&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_plot_norxn.png]]      [[File:Contour_norxn.png]]&lt;br /&gt;
&lt;br /&gt;
To find the transition state, the surface (above, on the left) and contour (above, on the right) plots were displayed. At a transition state, only a single black dot can been seen on a surface plot as there is no trajectory. Moreover, the contour plot was left blank, as the reaction did not happen, but no oscillation is observed as the vibrational freedom of the complex is being retained. The transition state was obtained at H-H distance: 0.745 Å, and H-F distance: 1.808 Å.&lt;br /&gt;
&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 Activation Energies &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Using the Energy vs Time plots, the following values have been established:&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F → HF + H:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -103.913 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 0.226 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -132.455 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 28.768 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Mechanisms of energy release&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
A scenario was set up in which the Animation and Momenta vs Time plots show that the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; - F reaction goes to completion. B and C were the H and A was the F atoms, with distances of A-B 1.5 Å, and B-C 0.878 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:mom_vs_time_AB_1.5_BC_0.878.png]]&lt;br /&gt;
&lt;br /&gt;
When the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule collides with the F atom, the translational energy of the species (due to the attraction between them) is being transformed into vibrational energy (oscillation being observed). Depending on the nature of the experiment, exothermic reactions release whereas, endothermic reactions absorb energy (in the form of heat) from the environment. When the oscillating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (both) atom approaches the  F atom (only translational energy), oscillation in the form of vibrational energy is being transmitted to the residual HF molecule. This way, the energy of the system is constant but the vibrational and kinetic energies are being transformed in between species. This can be confirmed experimentally by measuring the vibrational energy of the system via IR spectroscopy or use bomb calorimetry to determine the kinetic energy of the system  - which is directly proportional to the translational energy and its momentum. &lt;br /&gt;
&lt;br /&gt;
rHH = 0.74 Å, with a momentum pFH = -0.5, pHH in the range -3 to 3, rHF was set to 1.5 Å&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! pHH !! Level of Vibration of H-H bond !! Reaction &lt;br /&gt;
|-&lt;br /&gt;
| -3 || medium || transition state &lt;br /&gt;
|-&lt;br /&gt;
| -2.9 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.8 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.7 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.6 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.25 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
|  -2|| medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| -1 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 0 || strong|| yes &lt;br /&gt;
|-&lt;br /&gt;
| 1 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 1.5 || weak || transition state &lt;br /&gt;
|-&lt;br /&gt;
|  2 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.25  || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.3 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.4 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.6 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.7 ||  weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
|  2.8 || weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| 2.9  || weak || yes  &lt;br /&gt;
|-&lt;br /&gt;
| 3 || medium || yes &lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction goes to completion between the values -1.5 and 1, 2.5-2.6 and 2.9-3.0. As a conclusion, it was determined that no certain trends can be depicted from the data which would link the momentum, the outcome and the stretch of vibrations together. Moreover, the reactions at 2.9 and 3.0 are against Polanyi&#039;s empirical rule.&lt;br /&gt;
&lt;br /&gt;
For a separate calculation, the same initial positions were used, for HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F  with rHH=0.74 A but the momentum of HF was changed to p= -0.8 and the HH momentum was 0.1. The reaction goes to completion and thus the reaction is valid!&lt;br /&gt;
&lt;br /&gt;
If we look at the Momenta vs Time plot, we can see a continuously oscillating path, hence the reaction had reached its end. A large momentum contribution is seen as a a result of a large contribution from the very strong HF bond. &lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; 2 Å&lt;br /&gt;
HF 0.893325 Å&lt;br /&gt;
Phh - 8&lt;br /&gt;
Phf -0,02&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5 Polanyi&#039;s Empirical Rule and the Distribution of Energy &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Polany&#039;s empirical rules&amp;lt;ref name=&amp;quot;No.2&amp;quot; /&amp;gt; are reflecting on the effect of transition states energetically different modes. An exothermic reaction - in which the products are higher in energy - the transition state is described as &#039;early&#039; as it is closer in energy to the reactants. Hence, the translational energy has a greater impact on the activated complex snd thus the reaction then the vibrational energy. Empirically, for an endothermic reaction -  with a corresponding late transition state - the vibrational energy has a greater importance on the reaction.&lt;br /&gt;
&lt;br /&gt;
In this case, &lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H&lt;br /&gt;
&lt;br /&gt;
is an exothermic reaction. Therefore, as described above it has an early transition state which suggest a greater impact from the translational energy contribution. The vibrational energy can be seen through the oscillating nature of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, where the translational contribution is largely coming from the H-F bond (both can be seen through their momenta). The effect of HH momentum is low. Therefore, larger HF contribution (momentum) would increase the chances of the reaction being completed. The experiment has failed to show a specific trend which would also comply with the theory. The results at 2.9 and 3 violate Polanyi&#039;s rules as discussed in the previous question. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.1&amp;quot;&amp;gt;T. Bligaard, J.K. Nørskov, in Chemical Bonding at Surfaces and Interfaces, 2008&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.2&amp;quot;&amp;gt;Polanyi, J. C. Concepts in Reaction Dynamics Acc. Chem. Res. 1972, 5, 161– 168&amp;lt;/ref&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793684</id>
		<title>MRD:MToth96</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793684"/>
		<updated>2019-05-28T11:08:17Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /*  Q2 Locating Transition States */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Collision of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Potential Energy Surface&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
 [[File:Surface_Plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface (&#039;&#039;see above&#039;&#039;), the transition state is found and defined as the point where it is true that ∂V(ri)/∂ri=0, and ∂V2(ri)/∂ri2&amp;gt;0.                       &lt;br /&gt;
Empirically, the gradient of the surface is hence equals zero. Looking at the surface plot, the kinetic energy surface, as a function of AB distance has &lt;br /&gt;
a curvature that describes the potential energy as a function of distance. The transition state is at its minimum, as the distances are in balance. &lt;br /&gt;
Also, the trajectory (see black line) has to have its maximum value at the transition state, as we are expecting an energy maximum at this point. &lt;br /&gt;
The transition state is the highest point along the trajectory. At this point, AB and BC are also equal. After the second differentiation, a local maximum &lt;br /&gt;
is found if the derived value is positive. It is distinguished from other local minima by implementing the following criterium: ∂V/dq1 = 0 and ∂V/dq2 = 0, &lt;br /&gt;
where q1 is the tangent to the minimum and q2 is orthogonal to this as well as to the reaction path. Hence, ∂V2/dq12 &amp;lt; 0 and ∂V2/dq22 &amp;gt; 0 for that point.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This isn&#039;t quite correct. The transition state is both a maximum and a minimum, in different directions. In the direction of the minimum energy trajectory (i.e. the path the black line follows) it is a maximum. The second partial derivative of a maximum is always negative. Therefore the second partial derivative of the function of the PES in the direction of the reaction trajectory will be negative. However, as the TS occurs on the minimum energy pathway, this point is also a minimum, but in a direction orthogonal to the reaction trajectory. Therefore, as the second partial derivative of a minimum is always positive, the second partial derivative of the PES at the TS in the direction orthogonal to the trajectory will be positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:04, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Locating Transition States&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
When the transition state is reached, both the AB and BC distances are equal. Atoms show no vibration and therefore the graph displays no straight lines in accordance with this observation. The optimal distance was found to be 0.908 Å, at which both AB and BC distances were equal. Also, the momentum for both p1 and p2 were set to zero. &lt;br /&gt;
The Intermolecular distanced vs Time plot is shown below (on the left). The aim was to minimise oscillation and obtain flat lines with no corresponding gradients. No vibration means no change in distance and the vibration of the H atom and molecule is restricted. A restriction in vibrational freedom means that the TS is reached. Moreover, the BC and AB distances are equal and the corresponding lines are on top of each other. A static picture of the animation of the transition state can be seen below (on the right)&lt;br /&gt;
&lt;br /&gt;
[[File:Diastance_vs_time_h2.PNG]] .     [[File:Animation_h2_static.PNG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Why does a restriction in vibrational freedom mean that the TS is reached? Also be careful - the distance AB=BC at the TS only for a symmetrical reaction and that is only because reactants = products. This is not true of any TS. Perhaps you are aware of this, but you need to state it explicitly in order for this statement to be true. I also do not understand your point stating that &amp;quot;the graph displays no straight lines&amp;quot; where there is no vibration. What straight lines? In order to be very clear about what you mean, you need to explain every point you make thoroughly.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:07, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 MEP and Dynamic Trajectory&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_mep.PNG]] .     [[File:Surface_dynamic.PNG]]&lt;br /&gt;
&lt;br /&gt;
The trajectory is displayed as the black line along the bottom of the surface plots (&#039;&#039;see above&#039;&#039;. When the MEP calculation (on the left) is used, the line starts from the transition state but is only displayed for a short length. Whereas, the dynamic calculation (on the right) gives a much longer, complete black trajectory. The program tries to find the steepest descent along the potential energy surface to obtained a minimum. The MEP method is being reset to zero after every step, whilst with dynamic calculation the data is being carried further to the next step. Hence, the calculation is being carried on regardless, whereas with MEP the kinetic energy stays at its minimum. Thus, an oscillating line with the dynamic, and a local maximum with the MEP calculation is being observed. &lt;br /&gt;
&lt;br /&gt;
[[File:normal.PNG]]               [[File:Changed_distance.PNG]]&lt;br /&gt;
&lt;br /&gt;
For comparison, values of interatomic distances were changed (&#039;&#039;see above&#039;&#039;. Values were being shifted from r1=ts+0.01, r2=ts (on the left); to r1=ts and r2=ts+0.01 (on the right)&lt;br /&gt;
In both cases, it was observed that the lines corresponding to the AB and BC distances were exchanged (as expected). When the numbers got changed, the transition state was approached by the opposite direction - as a symmetrical system is being considered - and the values are exactly the same but opposite. Hence, the same plot was displayed in the opposite direction. The same variations were applied for Momenta vs Time plots. The observations are exactly the same as for the distances, with the position of the lines being exchanged in between. The initial values are displayed below on the left, whereas the changed values can be seen on the right.&lt;br /&gt;
&lt;br /&gt;
[[File:Normal_momentum.PNG]]         [[File:Changed.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Reactivity through trajectory analysis &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; (kcal.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;
| -1.25 || -2.5  || -99.018 || Yes || A-B oscillates, B and C bond formation || [[File:-1.25,-2.5_p1,p2.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  || -100.456 || No || A-B oscillates, no reaction || [[File:-1.5,-2.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  || -98.956 || Yes || A-B oscillates, B and C bond formation || [[File:-1.5,-2.5.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  || -84.956 || No ||  A-B oscillates intensely, B and C bond formation is expected, but it bounces off and C remains a single atom || [[File:-2.5,-5.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  || -83.416 || Yes || 	A-B oscillates intensely, very close transition state, B and C bond formation || [[File:-2.5,-5.2.png]]&lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
From the table above it was concluded that the E total of the system depends on the momentum. Moreover, it shows a correlation with the kinetic energy of the system. The potential energy is constant and the kinetic energy is changing in response the structural changes. Furthermore, the system&#039;s susceptibility to undergo a reaction is also dependent on the momentum (not just on energy). If there is a large momentum difference between the single atom and the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule - especially when the incoming atom&#039;s momentum is marginally lower - than the reaction will not happen.&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5  Transition State Theory &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Transition State theory&amp;lt;ref name=&amp;quot;No.1&amp;quot; /&amp;gt; is a way of describing chemical reactions as such that the reaction consist of atoms and molecules are subjected to a continuous change in the energies and positions. The transition state is being described as the position along the reaction path where the energy is at its maximum. The activation energy corresponding to a specific reaction and to its reactant is the energy necessary to initiate collisions sufficient to reach the transition state. It is calculated as the difference between the reactants and the transition state. The transition state or activated complex is in equilibrium with the reactant and hence its properties can be approximated using Hammond&#039;s postulate. Moreover, the rate if reaction - formation of products - can be approximates from the concentration of these activated complexes and their ability to go to completion.&lt;br /&gt;
&lt;br /&gt;
Furthermore, the transition state theory can also be applied to the quasi-equilibrium state. The reactants are in equilibrium with the transition state complex. This means that an equilibrium is always established in between the reactant and the activated complex regardless of the relationship of the reactant and the product (if they are in equilibrium). This part of the theory can be materialised in the form of a mathematical expression through the Van Hoff equation. The equation describes an equilibrium state, which is reversible and temperature dependent. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{d\ln K}{dT} = \frac{\Delta U}{RT^{2}}&amp;lt;/math&amp;gt;    &#039;&#039;where, K - eq. constant, T - temperature in K, U - internal energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In order to get the temperature dependence of reaction rates, the equation is derived and as a result the Arrhenius equation is being formulated. The Arrhenius equation shows the temperature dependence of reaction rates as well as the activation energy of a corresponding reaction.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;k = Ae^{-E_a/RT}&amp;lt;/math&amp;gt;     &#039;&#039;where k - rate constant, T - temperature in K, A - exponential factor, Ea - activation energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
According to the theory, the last reaction -  where P1 and P2 were -2.5 and -5.0 respectively - must go to completion. However, the exact opposite was observed. As a conclusion, it is suggested that the rate constant is lower in real life than it is in theory. Therefore, the rate constant prevents the reaction from going to completion. (the energy barrier is sufficient to retain AB as a molecule when is it being subjected to a collision by C)&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;System of F-H-H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Classification of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:FH_E_surface.png]]&lt;br /&gt;
&lt;br /&gt;
Atoms A and B are H-s, whereas C was F. The surface plot (&#039;&#039;see above&#039;&#039;) shows that the reactants (on the right hand side) are higher in energy than the product (on the left hand side). Therefore the reaction:&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H &lt;br /&gt;
&lt;br /&gt;
is exothermic (negative sign, accompanied by a decrease in energy). Hence the reverse reaction: &lt;br /&gt;
&lt;br /&gt;
H + HF → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F&lt;br /&gt;
&lt;br /&gt;
must be endothermic, as this is the corresponding backward reaction. In that case, the reactants will be lower in energy and the products will be higher. Additional energy is required to pass the activation energy barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:HF_surfce_endothemic.png]] &lt;br /&gt;
&lt;br /&gt;
The first reaction is exothermic, (bond making is exothermic) which means that the final product will be in a lower energy state than the reactants. Hence, the HF bond is a stronger bond and is lower in energy than the H-H bond. This is due to the ionic nature of the H-F bond due to a large difference in electronegativity. The surface plot of the endothermic reaction is shown above. It can be depicted that the reactant are in a lower energy state than the product.&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Position of the Transition State&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_plot_norxn.png]]      [[File:Contour_norxn.png]]&lt;br /&gt;
&lt;br /&gt;
To find the transition state, the surface (above, on the left) and contour (above, on the right) plots were displayed. At a transition state, only a single black dot can been seen on a surface plot as there is no trajectory. Moreover, the contour plot was left blank, as the reaction did not happen, but no oscillation is observed as the vibrational freedom of the complex is being retained. The transition state was obtained at H-H distance: 0.745 Å, and H-F distance: 1.808 Å.&lt;br /&gt;
&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 Activation Energies &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Using the Energy vs Time plots, the following values have been established:&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F → HF + H:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -103.913 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 0.226 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -132.455 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 28.768 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Mechanisms of energy release&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
A scenario was set up in which the Animation and Momenta vs Time plots show that the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; - F reaction goes to completion. B and C were the H and A was the F atoms, with distances of A-B 1.5 Å, and B-C 0.878 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:mom_vs_time_AB_1.5_BC_0.878.png]]&lt;br /&gt;
&lt;br /&gt;
When the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule collides with the F atom, the translational energy of the species (due to the attraction between them) is being transformed into vibrational energy (oscillation being observed). Depending on the nature of the experiment, exothermic reactions release whereas, endothermic reactions absorb energy (in the form of heat) from the environment. When the oscillating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (both) atom approaches the  F atom (only translational energy), oscillation in the form of vibrational energy is being transmitted to the residual HF molecule. This way, the energy of the system is constant but the vibrational and kinetic energies are being transformed in between species. This can be confirmed experimentally by measuring the vibrational energy of the system via IR spectroscopy or use bomb calorimetry to determine the kinetic energy of the system  - which is directly proportional to the translational energy and its momentum. &lt;br /&gt;
&lt;br /&gt;
rHH = 0.74 Å, with a momentum pFH = -0.5, pHH in the range -3 to 3, rHF was set to 1.5 Å&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! pHH !! Level of Vibration of H-H bond !! Reaction &lt;br /&gt;
|-&lt;br /&gt;
| -3 || medium || transition state &lt;br /&gt;
|-&lt;br /&gt;
| -2.9 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.8 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.7 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.6 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.25 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
|  -2|| medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| -1 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 0 || strong|| yes &lt;br /&gt;
|-&lt;br /&gt;
| 1 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 1.5 || weak || transition state &lt;br /&gt;
|-&lt;br /&gt;
|  2 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.25  || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.3 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.4 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.6 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.7 ||  weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
|  2.8 || weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| 2.9  || weak || yes  &lt;br /&gt;
|-&lt;br /&gt;
| 3 || medium || yes &lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction goes to completion between the values -1.5 and 1, 2.5-2.6 and 2.9-3.0. As a conclusion, it was determined that no certain trends can be depicted from the data which would link the momentum, the outcome and the stretch of vibrations together. Moreover, the reactions at 2.9 and 3.0 are against Polanyi&#039;s empirical rule.&lt;br /&gt;
&lt;br /&gt;
For a separate calculation, the same initial positions were used, for HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F  with rHH=0.74 A but the momentum of HF was changed to p= -0.8 and the HH momentum was 0.1. The reaction goes to completion and thus the reaction is valid!&lt;br /&gt;
&lt;br /&gt;
If we look at the Momenta vs Time plot, we can see a continuously oscillating path, hence the reaction had reached its end. A large momentum contribution is seen as a a result of a large contribution from the very strong HF bond. &lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; 2 Å&lt;br /&gt;
HF 0.893325 Å&lt;br /&gt;
Phh - 8&lt;br /&gt;
Phf -0,02&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5 Polanyi&#039;s Empirical Rule and the Distribution of Energy &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Polany&#039;s empirical rules&amp;lt;ref name=&amp;quot;No.2&amp;quot; /&amp;gt; are reflecting on the effect of transition states energetically different modes. An exothermic reaction - in which the products are higher in energy - the transition state is described as &#039;early&#039; as it is closer in energy to the reactants. Hence, the translational energy has a greater impact on the activated complex snd thus the reaction then the vibrational energy. Empirically, for an endothermic reaction -  with a corresponding late transition state - the vibrational energy has a greater importance on the reaction.&lt;br /&gt;
&lt;br /&gt;
In this case, &lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H&lt;br /&gt;
&lt;br /&gt;
is an exothermic reaction. Therefore, as described above it has an early transition state which suggest a greater impact from the translational energy contribution. The vibrational energy can be seen through the oscillating nature of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, where the translational contribution is largely coming from the H-F bond (both can be seen through their momenta). The effect of HH momentum is low. Therefore, larger HF contribution (momentum) would increase the chances of the reaction being completed. The experiment has failed to show a specific trend which would also comply with the theory. The results at 2.9 and 3 violate Polanyi&#039;s rules as discussed in the previous question. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.1&amp;quot;&amp;gt;T. Bligaard, J.K. Nørskov, in Chemical Bonding at Surfaces and Interfaces, 2008&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.2&amp;quot;&amp;gt;Polanyi, J. C. Concepts in Reaction Dynamics Acc. Chem. Res. 1972, 5, 161– 168&amp;lt;/ref&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793683</id>
		<title>MRD:MToth96</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793683"/>
		<updated>2019-05-28T11:07:45Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /*  Q2 Locating Transition States */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Collision of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Potential Energy Surface&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
 [[File:Surface_Plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface (&#039;&#039;see above&#039;&#039;), the transition state is found and defined as the point where it is true that ∂V(ri)/∂ri=0, and ∂V2(ri)/∂ri2&amp;gt;0.                       &lt;br /&gt;
Empirically, the gradient of the surface is hence equals zero. Looking at the surface plot, the kinetic energy surface, as a function of AB distance has &lt;br /&gt;
a curvature that describes the potential energy as a function of distance. The transition state is at its minimum, as the distances are in balance. &lt;br /&gt;
Also, the trajectory (see black line) has to have its maximum value at the transition state, as we are expecting an energy maximum at this point. &lt;br /&gt;
The transition state is the highest point along the trajectory. At this point, AB and BC are also equal. After the second differentiation, a local maximum &lt;br /&gt;
is found if the derived value is positive. It is distinguished from other local minima by implementing the following criterium: ∂V/dq1 = 0 and ∂V/dq2 = 0, &lt;br /&gt;
where q1 is the tangent to the minimum and q2 is orthogonal to this as well as to the reaction path. Hence, ∂V2/dq12 &amp;lt; 0 and ∂V2/dq22 &amp;gt; 0 for that point.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This isn&#039;t quite correct. The transition state is both a maximum and a minimum, in different directions. In the direction of the minimum energy trajectory (i.e. the path the black line follows) it is a maximum. The second partial derivative of a maximum is always negative. Therefore the second partial derivative of the function of the PES in the direction of the reaction trajectory will be negative. However, as the TS occurs on the minimum energy pathway, this point is also a minimum, but in a direction orthogonal to the reaction trajectory. Therefore, as the second partial derivative of a minimum is always positive, the second partial derivative of the PES at the TS in the direction orthogonal to the trajectory will be positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:04, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Locating Transition States&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
When the transition state is reached, both the AB and BC distances are equal. Atoms show no vibration and therefore the graph displays no straight lines in accordance with this observation. The optimal distance was found to be 0.908 Å, at which both AB and BC distances were equal. Also, the momentum for both p1 and p2 were set to zero. &lt;br /&gt;
The Intermolecular distanced vs Time plot is shown below (on the left). The aim was to minimise oscillation and obtain flat lines with no corresponding gradients. No vibration means no change in distance and the vibration of the H atom and molecule is restricted. A restriction in vibrational freedom means that the TS is reached. Moreover, the BC and AB distances are equal and the corresponding lines are on top of each other. A static picture of the animation of the transition state can be seen below (on the right)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Why does a restriction in vibrational freedom mean that the TS is reached? Also be careful - the distance AB=BC at the TS only for a symmetrical reaction and that is only because reactants = products. This is not true of any TS. I also do not understand your point stating that &amp;quot;the graph displays no straight lines&amp;quot; where there is no vibration. What straight lines? In order to be very clear about what you mean, you need to explain every point you make thoroughly.[[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:07, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
[[File:Diastance_vs_time_h2.PNG]] .     [[File:Animation_h2_static.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 MEP and Dynamic Trajectory&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_mep.PNG]] .     [[File:Surface_dynamic.PNG]]&lt;br /&gt;
&lt;br /&gt;
The trajectory is displayed as the black line along the bottom of the surface plots (&#039;&#039;see above&#039;&#039;. When the MEP calculation (on the left) is used, the line starts from the transition state but is only displayed for a short length. Whereas, the dynamic calculation (on the right) gives a much longer, complete black trajectory. The program tries to find the steepest descent along the potential energy surface to obtained a minimum. The MEP method is being reset to zero after every step, whilst with dynamic calculation the data is being carried further to the next step. Hence, the calculation is being carried on regardless, whereas with MEP the kinetic energy stays at its minimum. Thus, an oscillating line with the dynamic, and a local maximum with the MEP calculation is being observed. &lt;br /&gt;
&lt;br /&gt;
[[File:normal.PNG]]               [[File:Changed_distance.PNG]]&lt;br /&gt;
&lt;br /&gt;
For comparison, values of interatomic distances were changed (&#039;&#039;see above&#039;&#039;. Values were being shifted from r1=ts+0.01, r2=ts (on the left); to r1=ts and r2=ts+0.01 (on the right)&lt;br /&gt;
In both cases, it was observed that the lines corresponding to the AB and BC distances were exchanged (as expected). When the numbers got changed, the transition state was approached by the opposite direction - as a symmetrical system is being considered - and the values are exactly the same but opposite. Hence, the same plot was displayed in the opposite direction. The same variations were applied for Momenta vs Time plots. The observations are exactly the same as for the distances, with the position of the lines being exchanged in between. The initial values are displayed below on the left, whereas the changed values can be seen on the right.&lt;br /&gt;
&lt;br /&gt;
[[File:Normal_momentum.PNG]]         [[File:Changed.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Reactivity through trajectory analysis &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; (kcal.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;
| -1.25 || -2.5  || -99.018 || Yes || A-B oscillates, B and C bond formation || [[File:-1.25,-2.5_p1,p2.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  || -100.456 || No || A-B oscillates, no reaction || [[File:-1.5,-2.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  || -98.956 || Yes || A-B oscillates, B and C bond formation || [[File:-1.5,-2.5.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  || -84.956 || No ||  A-B oscillates intensely, B and C bond formation is expected, but it bounces off and C remains a single atom || [[File:-2.5,-5.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  || -83.416 || Yes || 	A-B oscillates intensely, very close transition state, B and C bond formation || [[File:-2.5,-5.2.png]]&lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
From the table above it was concluded that the E total of the system depends on the momentum. Moreover, it shows a correlation with the kinetic energy of the system. The potential energy is constant and the kinetic energy is changing in response the structural changes. Furthermore, the system&#039;s susceptibility to undergo a reaction is also dependent on the momentum (not just on energy). If there is a large momentum difference between the single atom and the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule - especially when the incoming atom&#039;s momentum is marginally lower - than the reaction will not happen.&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5  Transition State Theory &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Transition State theory&amp;lt;ref name=&amp;quot;No.1&amp;quot; /&amp;gt; is a way of describing chemical reactions as such that the reaction consist of atoms and molecules are subjected to a continuous change in the energies and positions. The transition state is being described as the position along the reaction path where the energy is at its maximum. The activation energy corresponding to a specific reaction and to its reactant is the energy necessary to initiate collisions sufficient to reach the transition state. It is calculated as the difference between the reactants and the transition state. The transition state or activated complex is in equilibrium with the reactant and hence its properties can be approximated using Hammond&#039;s postulate. Moreover, the rate if reaction - formation of products - can be approximates from the concentration of these activated complexes and their ability to go to completion.&lt;br /&gt;
&lt;br /&gt;
Furthermore, the transition state theory can also be applied to the quasi-equilibrium state. The reactants are in equilibrium with the transition state complex. This means that an equilibrium is always established in between the reactant and the activated complex regardless of the relationship of the reactant and the product (if they are in equilibrium). This part of the theory can be materialised in the form of a mathematical expression through the Van Hoff equation. The equation describes an equilibrium state, which is reversible and temperature dependent. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{d\ln K}{dT} = \frac{\Delta U}{RT^{2}}&amp;lt;/math&amp;gt;    &#039;&#039;where, K - eq. constant, T - temperature in K, U - internal energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In order to get the temperature dependence of reaction rates, the equation is derived and as a result the Arrhenius equation is being formulated. The Arrhenius equation shows the temperature dependence of reaction rates as well as the activation energy of a corresponding reaction.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;k = Ae^{-E_a/RT}&amp;lt;/math&amp;gt;     &#039;&#039;where k - rate constant, T - temperature in K, A - exponential factor, Ea - activation energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
According to the theory, the last reaction -  where P1 and P2 were -2.5 and -5.0 respectively - must go to completion. However, the exact opposite was observed. As a conclusion, it is suggested that the rate constant is lower in real life than it is in theory. Therefore, the rate constant prevents the reaction from going to completion. (the energy barrier is sufficient to retain AB as a molecule when is it being subjected to a collision by C)&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;System of F-H-H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Classification of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:FH_E_surface.png]]&lt;br /&gt;
&lt;br /&gt;
Atoms A and B are H-s, whereas C was F. The surface plot (&#039;&#039;see above&#039;&#039;) shows that the reactants (on the right hand side) are higher in energy than the product (on the left hand side). Therefore the reaction:&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H &lt;br /&gt;
&lt;br /&gt;
is exothermic (negative sign, accompanied by a decrease in energy). Hence the reverse reaction: &lt;br /&gt;
&lt;br /&gt;
H + HF → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F&lt;br /&gt;
&lt;br /&gt;
must be endothermic, as this is the corresponding backward reaction. In that case, the reactants will be lower in energy and the products will be higher. Additional energy is required to pass the activation energy barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:HF_surfce_endothemic.png]] &lt;br /&gt;
&lt;br /&gt;
The first reaction is exothermic, (bond making is exothermic) which means that the final product will be in a lower energy state than the reactants. Hence, the HF bond is a stronger bond and is lower in energy than the H-H bond. This is due to the ionic nature of the H-F bond due to a large difference in electronegativity. The surface plot of the endothermic reaction is shown above. It can be depicted that the reactant are in a lower energy state than the product.&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Position of the Transition State&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_plot_norxn.png]]      [[File:Contour_norxn.png]]&lt;br /&gt;
&lt;br /&gt;
To find the transition state, the surface (above, on the left) and contour (above, on the right) plots were displayed. At a transition state, only a single black dot can been seen on a surface plot as there is no trajectory. Moreover, the contour plot was left blank, as the reaction did not happen, but no oscillation is observed as the vibrational freedom of the complex is being retained. The transition state was obtained at H-H distance: 0.745 Å, and H-F distance: 1.808 Å.&lt;br /&gt;
&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 Activation Energies &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Using the Energy vs Time plots, the following values have been established:&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F → HF + H:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -103.913 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 0.226 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -132.455 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 28.768 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Mechanisms of energy release&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
A scenario was set up in which the Animation and Momenta vs Time plots show that the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; - F reaction goes to completion. B and C were the H and A was the F atoms, with distances of A-B 1.5 Å, and B-C 0.878 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:mom_vs_time_AB_1.5_BC_0.878.png]]&lt;br /&gt;
&lt;br /&gt;
When the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule collides with the F atom, the translational energy of the species (due to the attraction between them) is being transformed into vibrational energy (oscillation being observed). Depending on the nature of the experiment, exothermic reactions release whereas, endothermic reactions absorb energy (in the form of heat) from the environment. When the oscillating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (both) atom approaches the  F atom (only translational energy), oscillation in the form of vibrational energy is being transmitted to the residual HF molecule. This way, the energy of the system is constant but the vibrational and kinetic energies are being transformed in between species. This can be confirmed experimentally by measuring the vibrational energy of the system via IR spectroscopy or use bomb calorimetry to determine the kinetic energy of the system  - which is directly proportional to the translational energy and its momentum. &lt;br /&gt;
&lt;br /&gt;
rHH = 0.74 Å, with a momentum pFH = -0.5, pHH in the range -3 to 3, rHF was set to 1.5 Å&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! pHH !! Level of Vibration of H-H bond !! Reaction &lt;br /&gt;
|-&lt;br /&gt;
| -3 || medium || transition state &lt;br /&gt;
|-&lt;br /&gt;
| -2.9 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.8 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.7 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.6 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.25 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
|  -2|| medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| -1 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 0 || strong|| yes &lt;br /&gt;
|-&lt;br /&gt;
| 1 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 1.5 || weak || transition state &lt;br /&gt;
|-&lt;br /&gt;
|  2 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.25  || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.3 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.4 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.6 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.7 ||  weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
|  2.8 || weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| 2.9  || weak || yes  &lt;br /&gt;
|-&lt;br /&gt;
| 3 || medium || yes &lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction goes to completion between the values -1.5 and 1, 2.5-2.6 and 2.9-3.0. As a conclusion, it was determined that no certain trends can be depicted from the data which would link the momentum, the outcome and the stretch of vibrations together. Moreover, the reactions at 2.9 and 3.0 are against Polanyi&#039;s empirical rule.&lt;br /&gt;
&lt;br /&gt;
For a separate calculation, the same initial positions were used, for HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F  with rHH=0.74 A but the momentum of HF was changed to p= -0.8 and the HH momentum was 0.1. The reaction goes to completion and thus the reaction is valid!&lt;br /&gt;
&lt;br /&gt;
If we look at the Momenta vs Time plot, we can see a continuously oscillating path, hence the reaction had reached its end. A large momentum contribution is seen as a a result of a large contribution from the very strong HF bond. &lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; 2 Å&lt;br /&gt;
HF 0.893325 Å&lt;br /&gt;
Phh - 8&lt;br /&gt;
Phf -0,02&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5 Polanyi&#039;s Empirical Rule and the Distribution of Energy &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Polany&#039;s empirical rules&amp;lt;ref name=&amp;quot;No.2&amp;quot; /&amp;gt; are reflecting on the effect of transition states energetically different modes. An exothermic reaction - in which the products are higher in energy - the transition state is described as &#039;early&#039; as it is closer in energy to the reactants. Hence, the translational energy has a greater impact on the activated complex snd thus the reaction then the vibrational energy. Empirically, for an endothermic reaction -  with a corresponding late transition state - the vibrational energy has a greater importance on the reaction.&lt;br /&gt;
&lt;br /&gt;
In this case, &lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H&lt;br /&gt;
&lt;br /&gt;
is an exothermic reaction. Therefore, as described above it has an early transition state which suggest a greater impact from the translational energy contribution. The vibrational energy can be seen through the oscillating nature of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, where the translational contribution is largely coming from the H-F bond (both can be seen through their momenta). The effect of HH momentum is low. Therefore, larger HF contribution (momentum) would increase the chances of the reaction being completed. The experiment has failed to show a specific trend which would also comply with the theory. The results at 2.9 and 3 violate Polanyi&#039;s rules as discussed in the previous question. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.1&amp;quot;&amp;gt;T. Bligaard, J.K. Nørskov, in Chemical Bonding at Surfaces and Interfaces, 2008&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.2&amp;quot;&amp;gt;Polanyi, J. C. Concepts in Reaction Dynamics Acc. Chem. Res. 1972, 5, 161– 168&amp;lt;/ref&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793682</id>
		<title>MRD:MToth96</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793682"/>
		<updated>2019-05-28T11:07:16Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /*  Q2 Locating Transition States */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Collision of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Potential Energy Surface&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
 [[File:Surface_Plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface (&#039;&#039;see above&#039;&#039;), the transition state is found and defined as the point where it is true that ∂V(ri)/∂ri=0, and ∂V2(ri)/∂ri2&amp;gt;0.                       &lt;br /&gt;
Empirically, the gradient of the surface is hence equals zero. Looking at the surface plot, the kinetic energy surface, as a function of AB distance has &lt;br /&gt;
a curvature that describes the potential energy as a function of distance. The transition state is at its minimum, as the distances are in balance. &lt;br /&gt;
Also, the trajectory (see black line) has to have its maximum value at the transition state, as we are expecting an energy maximum at this point. &lt;br /&gt;
The transition state is the highest point along the trajectory. At this point, AB and BC are also equal. After the second differentiation, a local maximum &lt;br /&gt;
is found if the derived value is positive. It is distinguished from other local minima by implementing the following criterium: ∂V/dq1 = 0 and ∂V/dq2 = 0, &lt;br /&gt;
where q1 is the tangent to the minimum and q2 is orthogonal to this as well as to the reaction path. Hence, ∂V2/dq12 &amp;lt; 0 and ∂V2/dq22 &amp;gt; 0 for that point.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This isn&#039;t quite correct. The transition state is both a maximum and a minimum, in different directions. In the direction of the minimum energy trajectory (i.e. the path the black line follows) it is a maximum. The second partial derivative of a maximum is always negative. Therefore the second partial derivative of the function of the PES in the direction of the reaction trajectory will be negative. However, as the TS occurs on the minimum energy pathway, this point is also a minimum, but in a direction orthogonal to the reaction trajectory. Therefore, as the second partial derivative of a minimum is always positive, the second partial derivative of the PES at the TS in the direction orthogonal to the trajectory will be positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:04, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Locating Transition States&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
When the transition state is reached, both the AB and BC distances are equal. Atoms show no vibration and therefore the graph displays no straight lines in accordance with this observation. The optimal distance was found to be 0.908 Å, at which both AB and BC distances were equal. Also, the momentum for both p1 and p2 were set to zero. &lt;br /&gt;
The Intermolecular distanced vs Time plot is shown below (on the left). The aim was to minimise oscillation and obtain flat lines with no corresponding gradients. No vibration means no change in distance and the vibration of the H atom and molecule is restricted. A restriction in vibrational freedom means that the TS is reached. Moreover, the BC and AB distances are equal and the corresponding lines are on top of each other. A static picture of the animation of the transition state can be seen below (on the right)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Why does a restriction in vibrational freedom mean that the TS is reached? Also be careful - the distance AB=BC at the TS only for a symmetrical reaction and that is only because reactants = products. This is not true of any TS. I also do not understand your point stating that &amp;quot;the graph displays no straight lines&amp;quot; where there is no vibration. What straight lines? In order to be very clear about what you mean, you need to explain every point you make thoroughly. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:06, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
[[File:Diastance_vs_time_h2.PNG]] .     [[File:Animation_h2_static.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 MEP and Dynamic Trajectory&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_mep.PNG]] .     [[File:Surface_dynamic.PNG]]&lt;br /&gt;
&lt;br /&gt;
The trajectory is displayed as the black line along the bottom of the surface plots (&#039;&#039;see above&#039;&#039;. When the MEP calculation (on the left) is used, the line starts from the transition state but is only displayed for a short length. Whereas, the dynamic calculation (on the right) gives a much longer, complete black trajectory. The program tries to find the steepest descent along the potential energy surface to obtained a minimum. The MEP method is being reset to zero after every step, whilst with dynamic calculation the data is being carried further to the next step. Hence, the calculation is being carried on regardless, whereas with MEP the kinetic energy stays at its minimum. Thus, an oscillating line with the dynamic, and a local maximum with the MEP calculation is being observed. &lt;br /&gt;
&lt;br /&gt;
[[File:normal.PNG]]               [[File:Changed_distance.PNG]]&lt;br /&gt;
&lt;br /&gt;
For comparison, values of interatomic distances were changed (&#039;&#039;see above&#039;&#039;. Values were being shifted from r1=ts+0.01, r2=ts (on the left); to r1=ts and r2=ts+0.01 (on the right)&lt;br /&gt;
In both cases, it was observed that the lines corresponding to the AB and BC distances were exchanged (as expected). When the numbers got changed, the transition state was approached by the opposite direction - as a symmetrical system is being considered - and the values are exactly the same but opposite. Hence, the same plot was displayed in the opposite direction. The same variations were applied for Momenta vs Time plots. The observations are exactly the same as for the distances, with the position of the lines being exchanged in between. The initial values are displayed below on the left, whereas the changed values can be seen on the right.&lt;br /&gt;
&lt;br /&gt;
[[File:Normal_momentum.PNG]]         [[File:Changed.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Reactivity through trajectory analysis &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; (kcal.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;
| -1.25 || -2.5  || -99.018 || Yes || A-B oscillates, B and C bond formation || [[File:-1.25,-2.5_p1,p2.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  || -100.456 || No || A-B oscillates, no reaction || [[File:-1.5,-2.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  || -98.956 || Yes || A-B oscillates, B and C bond formation || [[File:-1.5,-2.5.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  || -84.956 || No ||  A-B oscillates intensely, B and C bond formation is expected, but it bounces off and C remains a single atom || [[File:-2.5,-5.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  || -83.416 || Yes || 	A-B oscillates intensely, very close transition state, B and C bond formation || [[File:-2.5,-5.2.png]]&lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
From the table above it was concluded that the E total of the system depends on the momentum. Moreover, it shows a correlation with the kinetic energy of the system. The potential energy is constant and the kinetic energy is changing in response the structural changes. Furthermore, the system&#039;s susceptibility to undergo a reaction is also dependent on the momentum (not just on energy). If there is a large momentum difference between the single atom and the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule - especially when the incoming atom&#039;s momentum is marginally lower - than the reaction will not happen.&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5  Transition State Theory &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Transition State theory&amp;lt;ref name=&amp;quot;No.1&amp;quot; /&amp;gt; is a way of describing chemical reactions as such that the reaction consist of atoms and molecules are subjected to a continuous change in the energies and positions. The transition state is being described as the position along the reaction path where the energy is at its maximum. The activation energy corresponding to a specific reaction and to its reactant is the energy necessary to initiate collisions sufficient to reach the transition state. It is calculated as the difference between the reactants and the transition state. The transition state or activated complex is in equilibrium with the reactant and hence its properties can be approximated using Hammond&#039;s postulate. Moreover, the rate if reaction - formation of products - can be approximates from the concentration of these activated complexes and their ability to go to completion.&lt;br /&gt;
&lt;br /&gt;
Furthermore, the transition state theory can also be applied to the quasi-equilibrium state. The reactants are in equilibrium with the transition state complex. This means that an equilibrium is always established in between the reactant and the activated complex regardless of the relationship of the reactant and the product (if they are in equilibrium). This part of the theory can be materialised in the form of a mathematical expression through the Van Hoff equation. The equation describes an equilibrium state, which is reversible and temperature dependent. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{d\ln K}{dT} = \frac{\Delta U}{RT^{2}}&amp;lt;/math&amp;gt;    &#039;&#039;where, K - eq. constant, T - temperature in K, U - internal energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In order to get the temperature dependence of reaction rates, the equation is derived and as a result the Arrhenius equation is being formulated. The Arrhenius equation shows the temperature dependence of reaction rates as well as the activation energy of a corresponding reaction.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;k = Ae^{-E_a/RT}&amp;lt;/math&amp;gt;     &#039;&#039;where k - rate constant, T - temperature in K, A - exponential factor, Ea - activation energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
According to the theory, the last reaction -  where P1 and P2 were -2.5 and -5.0 respectively - must go to completion. However, the exact opposite was observed. As a conclusion, it is suggested that the rate constant is lower in real life than it is in theory. Therefore, the rate constant prevents the reaction from going to completion. (the energy barrier is sufficient to retain AB as a molecule when is it being subjected to a collision by C)&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;System of F-H-H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Classification of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:FH_E_surface.png]]&lt;br /&gt;
&lt;br /&gt;
Atoms A and B are H-s, whereas C was F. The surface plot (&#039;&#039;see above&#039;&#039;) shows that the reactants (on the right hand side) are higher in energy than the product (on the left hand side). Therefore the reaction:&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H &lt;br /&gt;
&lt;br /&gt;
is exothermic (negative sign, accompanied by a decrease in energy). Hence the reverse reaction: &lt;br /&gt;
&lt;br /&gt;
H + HF → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F&lt;br /&gt;
&lt;br /&gt;
must be endothermic, as this is the corresponding backward reaction. In that case, the reactants will be lower in energy and the products will be higher. Additional energy is required to pass the activation energy barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:HF_surfce_endothemic.png]] &lt;br /&gt;
&lt;br /&gt;
The first reaction is exothermic, (bond making is exothermic) which means that the final product will be in a lower energy state than the reactants. Hence, the HF bond is a stronger bond and is lower in energy than the H-H bond. This is due to the ionic nature of the H-F bond due to a large difference in electronegativity. The surface plot of the endothermic reaction is shown above. It can be depicted that the reactant are in a lower energy state than the product.&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Position of the Transition State&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_plot_norxn.png]]      [[File:Contour_norxn.png]]&lt;br /&gt;
&lt;br /&gt;
To find the transition state, the surface (above, on the left) and contour (above, on the right) plots were displayed. At a transition state, only a single black dot can been seen on a surface plot as there is no trajectory. Moreover, the contour plot was left blank, as the reaction did not happen, but no oscillation is observed as the vibrational freedom of the complex is being retained. The transition state was obtained at H-H distance: 0.745 Å, and H-F distance: 1.808 Å.&lt;br /&gt;
&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 Activation Energies &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Using the Energy vs Time plots, the following values have been established:&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F → HF + H:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -103.913 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 0.226 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -132.455 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 28.768 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Mechanisms of energy release&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
A scenario was set up in which the Animation and Momenta vs Time plots show that the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; - F reaction goes to completion. B and C were the H and A was the F atoms, with distances of A-B 1.5 Å, and B-C 0.878 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:mom_vs_time_AB_1.5_BC_0.878.png]]&lt;br /&gt;
&lt;br /&gt;
When the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule collides with the F atom, the translational energy of the species (due to the attraction between them) is being transformed into vibrational energy (oscillation being observed). Depending on the nature of the experiment, exothermic reactions release whereas, endothermic reactions absorb energy (in the form of heat) from the environment. When the oscillating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (both) atom approaches the  F atom (only translational energy), oscillation in the form of vibrational energy is being transmitted to the residual HF molecule. This way, the energy of the system is constant but the vibrational and kinetic energies are being transformed in between species. This can be confirmed experimentally by measuring the vibrational energy of the system via IR spectroscopy or use bomb calorimetry to determine the kinetic energy of the system  - which is directly proportional to the translational energy and its momentum. &lt;br /&gt;
&lt;br /&gt;
rHH = 0.74 Å, with a momentum pFH = -0.5, pHH in the range -3 to 3, rHF was set to 1.5 Å&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! pHH !! Level of Vibration of H-H bond !! Reaction &lt;br /&gt;
|-&lt;br /&gt;
| -3 || medium || transition state &lt;br /&gt;
|-&lt;br /&gt;
| -2.9 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.8 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.7 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.6 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.25 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
|  -2|| medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| -1 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 0 || strong|| yes &lt;br /&gt;
|-&lt;br /&gt;
| 1 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 1.5 || weak || transition state &lt;br /&gt;
|-&lt;br /&gt;
|  2 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.25  || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.3 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.4 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.6 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.7 ||  weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
|  2.8 || weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| 2.9  || weak || yes  &lt;br /&gt;
|-&lt;br /&gt;
| 3 || medium || yes &lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction goes to completion between the values -1.5 and 1, 2.5-2.6 and 2.9-3.0. As a conclusion, it was determined that no certain trends can be depicted from the data which would link the momentum, the outcome and the stretch of vibrations together. Moreover, the reactions at 2.9 and 3.0 are against Polanyi&#039;s empirical rule.&lt;br /&gt;
&lt;br /&gt;
For a separate calculation, the same initial positions were used, for HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F  with rHH=0.74 A but the momentum of HF was changed to p= -0.8 and the HH momentum was 0.1. The reaction goes to completion and thus the reaction is valid!&lt;br /&gt;
&lt;br /&gt;
If we look at the Momenta vs Time plot, we can see a continuously oscillating path, hence the reaction had reached its end. A large momentum contribution is seen as a a result of a large contribution from the very strong HF bond. &lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; 2 Å&lt;br /&gt;
HF 0.893325 Å&lt;br /&gt;
Phh - 8&lt;br /&gt;
Phf -0,02&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5 Polanyi&#039;s Empirical Rule and the Distribution of Energy &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Polany&#039;s empirical rules&amp;lt;ref name=&amp;quot;No.2&amp;quot; /&amp;gt; are reflecting on the effect of transition states energetically different modes. An exothermic reaction - in which the products are higher in energy - the transition state is described as &#039;early&#039; as it is closer in energy to the reactants. Hence, the translational energy has a greater impact on the activated complex snd thus the reaction then the vibrational energy. Empirically, for an endothermic reaction -  with a corresponding late transition state - the vibrational energy has a greater importance on the reaction.&lt;br /&gt;
&lt;br /&gt;
In this case, &lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H&lt;br /&gt;
&lt;br /&gt;
is an exothermic reaction. Therefore, as described above it has an early transition state which suggest a greater impact from the translational energy contribution. The vibrational energy can be seen through the oscillating nature of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, where the translational contribution is largely coming from the H-F bond (both can be seen through their momenta). The effect of HH momentum is low. Therefore, larger HF contribution (momentum) would increase the chances of the reaction being completed. The experiment has failed to show a specific trend which would also comply with the theory. The results at 2.9 and 3 violate Polanyi&#039;s rules as discussed in the previous question. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.1&amp;quot;&amp;gt;T. Bligaard, J.K. Nørskov, in Chemical Bonding at Surfaces and Interfaces, 2008&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.2&amp;quot;&amp;gt;Polanyi, J. C. Concepts in Reaction Dynamics Acc. Chem. Res. 1972, 5, 161– 168&amp;lt;/ref&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793681</id>
		<title>MRD:MToth96</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793681"/>
		<updated>2019-05-28T11:06:53Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /*  Q2 Locating Transition States */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Collision of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Potential Energy Surface&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
 [[File:Surface_Plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface (&#039;&#039;see above&#039;&#039;), the transition state is found and defined as the point where it is true that ∂V(ri)/∂ri=0, and ∂V2(ri)/∂ri2&amp;gt;0.                       &lt;br /&gt;
Empirically, the gradient of the surface is hence equals zero. Looking at the surface plot, the kinetic energy surface, as a function of AB distance has &lt;br /&gt;
a curvature that describes the potential energy as a function of distance. The transition state is at its minimum, as the distances are in balance. &lt;br /&gt;
Also, the trajectory (see black line) has to have its maximum value at the transition state, as we are expecting an energy maximum at this point. &lt;br /&gt;
The transition state is the highest point along the trajectory. At this point, AB and BC are also equal. After the second differentiation, a local maximum &lt;br /&gt;
is found if the derived value is positive. It is distinguished from other local minima by implementing the following criterium: ∂V/dq1 = 0 and ∂V/dq2 = 0, &lt;br /&gt;
where q1 is the tangent to the minimum and q2 is orthogonal to this as well as to the reaction path. Hence, ∂V2/dq12 &amp;lt; 0 and ∂V2/dq22 &amp;gt; 0 for that point.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This isn&#039;t quite correct. The transition state is both a maximum and a minimum, in different directions. In the direction of the minimum energy trajectory (i.e. the path the black line follows) it is a maximum. The second partial derivative of a maximum is always negative. Therefore the second partial derivative of the function of the PES in the direction of the reaction trajectory will be negative. However, as the TS occurs on the minimum energy pathway, this point is also a minimum, but in a direction orthogonal to the reaction trajectory. Therefore, as the second partial derivative of a minimum is always positive, the second partial derivative of the PES at the TS in the direction orthogonal to the trajectory will be positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:04, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Locating Transition States&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
When the transition state is reached, both the AB and BC distances are equal. Atoms show no vibration and therefore the graph displays no straight lines in accordance with this observation. The optimal distance was found to be 0.908 Å, at which both AB and BC distances were equal. Also, the momentum for both p1 and p2 were set to zero. &lt;br /&gt;
The Intermolecular distanced vs Time plot is shown below (on the left). The aim was to minimise oscillation and obtain flat lines with no corresponding gradients. No vibration means no change in distance and the vibration of the H atom and molecule is restricted. A restriction in vibrational freedom means that the TS is reached. Moreover, the BC and AB distances are equal and the corresponding lines are on top of each other. A static picture of the animation of the transition state can be seen below (on the right)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Why does a restriction in vibrational freedom mean that the TS is reached? Also be careful - the distance AB=BC at the TS only for a symmetrical reaction and that is only because reactants = products. This is not true of any TS. I also do not understand your point stating that &amp;quot;the graph displays no straight lines&amp;quot; where there is no vibration. What straight lines? In order to be very clear about what you mean, you need to explain every point you make thoroughly. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:06, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
[[File:Diastance_vs_time_h2.PNG]] .     [[File:Animation_h2_static.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 MEP and Dynamic Trajectory&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_mep.PNG]] .     [[File:Surface_dynamic.PNG]]&lt;br /&gt;
&lt;br /&gt;
The trajectory is displayed as the black line along the bottom of the surface plots (&#039;&#039;see above&#039;&#039;. When the MEP calculation (on the left) is used, the line starts from the transition state but is only displayed for a short length. Whereas, the dynamic calculation (on the right) gives a much longer, complete black trajectory. The program tries to find the steepest descent along the potential energy surface to obtained a minimum. The MEP method is being reset to zero after every step, whilst with dynamic calculation the data is being carried further to the next step. Hence, the calculation is being carried on regardless, whereas with MEP the kinetic energy stays at its minimum. Thus, an oscillating line with the dynamic, and a local maximum with the MEP calculation is being observed. &lt;br /&gt;
&lt;br /&gt;
[[File:normal.PNG]]               [[File:Changed_distance.PNG]]&lt;br /&gt;
&lt;br /&gt;
For comparison, values of interatomic distances were changed (&#039;&#039;see above&#039;&#039;. Values were being shifted from r1=ts+0.01, r2=ts (on the left); to r1=ts and r2=ts+0.01 (on the right)&lt;br /&gt;
In both cases, it was observed that the lines corresponding to the AB and BC distances were exchanged (as expected). When the numbers got changed, the transition state was approached by the opposite direction - as a symmetrical system is being considered - and the values are exactly the same but opposite. Hence, the same plot was displayed in the opposite direction. The same variations were applied for Momenta vs Time plots. The observations are exactly the same as for the distances, with the position of the lines being exchanged in between. The initial values are displayed below on the left, whereas the changed values can be seen on the right.&lt;br /&gt;
&lt;br /&gt;
[[File:Normal_momentum.PNG]]         [[File:Changed.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Reactivity through trajectory analysis &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; (kcal.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;
| -1.25 || -2.5  || -99.018 || Yes || A-B oscillates, B and C bond formation || [[File:-1.25,-2.5_p1,p2.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  || -100.456 || No || A-B oscillates, no reaction || [[File:-1.5,-2.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  || -98.956 || Yes || A-B oscillates, B and C bond formation || [[File:-1.5,-2.5.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  || -84.956 || No ||  A-B oscillates intensely, B and C bond formation is expected, but it bounces off and C remains a single atom || [[File:-2.5,-5.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  || -83.416 || Yes || 	A-B oscillates intensely, very close transition state, B and C bond formation || [[File:-2.5,-5.2.png]]&lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
From the table above it was concluded that the E total of the system depends on the momentum. Moreover, it shows a correlation with the kinetic energy of the system. The potential energy is constant and the kinetic energy is changing in response the structural changes. Furthermore, the system&#039;s susceptibility to undergo a reaction is also dependent on the momentum (not just on energy). If there is a large momentum difference between the single atom and the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule - especially when the incoming atom&#039;s momentum is marginally lower - than the reaction will not happen.&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5  Transition State Theory &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Transition State theory&amp;lt;ref name=&amp;quot;No.1&amp;quot; /&amp;gt; is a way of describing chemical reactions as such that the reaction consist of atoms and molecules are subjected to a continuous change in the energies and positions. The transition state is being described as the position along the reaction path where the energy is at its maximum. The activation energy corresponding to a specific reaction and to its reactant is the energy necessary to initiate collisions sufficient to reach the transition state. It is calculated as the difference between the reactants and the transition state. The transition state or activated complex is in equilibrium with the reactant and hence its properties can be approximated using Hammond&#039;s postulate. Moreover, the rate if reaction - formation of products - can be approximates from the concentration of these activated complexes and their ability to go to completion.&lt;br /&gt;
&lt;br /&gt;
Furthermore, the transition state theory can also be applied to the quasi-equilibrium state. The reactants are in equilibrium with the transition state complex. This means that an equilibrium is always established in between the reactant and the activated complex regardless of the relationship of the reactant and the product (if they are in equilibrium). This part of the theory can be materialised in the form of a mathematical expression through the Van Hoff equation. The equation describes an equilibrium state, which is reversible and temperature dependent. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{d\ln K}{dT} = \frac{\Delta U}{RT^{2}}&amp;lt;/math&amp;gt;    &#039;&#039;where, K - eq. constant, T - temperature in K, U - internal energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In order to get the temperature dependence of reaction rates, the equation is derived and as a result the Arrhenius equation is being formulated. The Arrhenius equation shows the temperature dependence of reaction rates as well as the activation energy of a corresponding reaction.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;k = Ae^{-E_a/RT}&amp;lt;/math&amp;gt;     &#039;&#039;where k - rate constant, T - temperature in K, A - exponential factor, Ea - activation energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
According to the theory, the last reaction -  where P1 and P2 were -2.5 and -5.0 respectively - must go to completion. However, the exact opposite was observed. As a conclusion, it is suggested that the rate constant is lower in real life than it is in theory. Therefore, the rate constant prevents the reaction from going to completion. (the energy barrier is sufficient to retain AB as a molecule when is it being subjected to a collision by C)&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;System of F-H-H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Classification of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:FH_E_surface.png]]&lt;br /&gt;
&lt;br /&gt;
Atoms A and B are H-s, whereas C was F. The surface plot (&#039;&#039;see above&#039;&#039;) shows that the reactants (on the right hand side) are higher in energy than the product (on the left hand side). Therefore the reaction:&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H &lt;br /&gt;
&lt;br /&gt;
is exothermic (negative sign, accompanied by a decrease in energy). Hence the reverse reaction: &lt;br /&gt;
&lt;br /&gt;
H + HF → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F&lt;br /&gt;
&lt;br /&gt;
must be endothermic, as this is the corresponding backward reaction. In that case, the reactants will be lower in energy and the products will be higher. Additional energy is required to pass the activation energy barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:HF_surfce_endothemic.png]] &lt;br /&gt;
&lt;br /&gt;
The first reaction is exothermic, (bond making is exothermic) which means that the final product will be in a lower energy state than the reactants. Hence, the HF bond is a stronger bond and is lower in energy than the H-H bond. This is due to the ionic nature of the H-F bond due to a large difference in electronegativity. The surface plot of the endothermic reaction is shown above. It can be depicted that the reactant are in a lower energy state than the product.&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Position of the Transition State&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_plot_norxn.png]]      [[File:Contour_norxn.png]]&lt;br /&gt;
&lt;br /&gt;
To find the transition state, the surface (above, on the left) and contour (above, on the right) plots were displayed. At a transition state, only a single black dot can been seen on a surface plot as there is no trajectory. Moreover, the contour plot was left blank, as the reaction did not happen, but no oscillation is observed as the vibrational freedom of the complex is being retained. The transition state was obtained at H-H distance: 0.745 Å, and H-F distance: 1.808 Å.&lt;br /&gt;
&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 Activation Energies &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Using the Energy vs Time plots, the following values have been established:&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F → HF + H:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -103.913 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 0.226 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -132.455 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 28.768 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Mechanisms of energy release&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
A scenario was set up in which the Animation and Momenta vs Time plots show that the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; - F reaction goes to completion. B and C were the H and A was the F atoms, with distances of A-B 1.5 Å, and B-C 0.878 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:mom_vs_time_AB_1.5_BC_0.878.png]]&lt;br /&gt;
&lt;br /&gt;
When the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule collides with the F atom, the translational energy of the species (due to the attraction between them) is being transformed into vibrational energy (oscillation being observed). Depending on the nature of the experiment, exothermic reactions release whereas, endothermic reactions absorb energy (in the form of heat) from the environment. When the oscillating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (both) atom approaches the  F atom (only translational energy), oscillation in the form of vibrational energy is being transmitted to the residual HF molecule. This way, the energy of the system is constant but the vibrational and kinetic energies are being transformed in between species. This can be confirmed experimentally by measuring the vibrational energy of the system via IR spectroscopy or use bomb calorimetry to determine the kinetic energy of the system  - which is directly proportional to the translational energy and its momentum. &lt;br /&gt;
&lt;br /&gt;
rHH = 0.74 Å, with a momentum pFH = -0.5, pHH in the range -3 to 3, rHF was set to 1.5 Å&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! pHH !! Level of Vibration of H-H bond !! Reaction &lt;br /&gt;
|-&lt;br /&gt;
| -3 || medium || transition state &lt;br /&gt;
|-&lt;br /&gt;
| -2.9 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.8 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.7 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.6 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.25 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
|  -2|| medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| -1 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 0 || strong|| yes &lt;br /&gt;
|-&lt;br /&gt;
| 1 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 1.5 || weak || transition state &lt;br /&gt;
|-&lt;br /&gt;
|  2 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.25  || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.3 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.4 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.6 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.7 ||  weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
|  2.8 || weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| 2.9  || weak || yes  &lt;br /&gt;
|-&lt;br /&gt;
| 3 || medium || yes &lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction goes to completion between the values -1.5 and 1, 2.5-2.6 and 2.9-3.0. As a conclusion, it was determined that no certain trends can be depicted from the data which would link the momentum, the outcome and the stretch of vibrations together. Moreover, the reactions at 2.9 and 3.0 are against Polanyi&#039;s empirical rule.&lt;br /&gt;
&lt;br /&gt;
For a separate calculation, the same initial positions were used, for HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F  with rHH=0.74 A but the momentum of HF was changed to p= -0.8 and the HH momentum was 0.1. The reaction goes to completion and thus the reaction is valid!&lt;br /&gt;
&lt;br /&gt;
If we look at the Momenta vs Time plot, we can see a continuously oscillating path, hence the reaction had reached its end. A large momentum contribution is seen as a a result of a large contribution from the very strong HF bond. &lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; 2 Å&lt;br /&gt;
HF 0.893325 Å&lt;br /&gt;
Phh - 8&lt;br /&gt;
Phf -0,02&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5 Polanyi&#039;s Empirical Rule and the Distribution of Energy &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Polany&#039;s empirical rules&amp;lt;ref name=&amp;quot;No.2&amp;quot; /&amp;gt; are reflecting on the effect of transition states energetically different modes. An exothermic reaction - in which the products are higher in energy - the transition state is described as &#039;early&#039; as it is closer in energy to the reactants. Hence, the translational energy has a greater impact on the activated complex snd thus the reaction then the vibrational energy. Empirically, for an endothermic reaction -  with a corresponding late transition state - the vibrational energy has a greater importance on the reaction.&lt;br /&gt;
&lt;br /&gt;
In this case, &lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H&lt;br /&gt;
&lt;br /&gt;
is an exothermic reaction. Therefore, as described above it has an early transition state which suggest a greater impact from the translational energy contribution. The vibrational energy can be seen through the oscillating nature of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, where the translational contribution is largely coming from the H-F bond (both can be seen through their momenta). The effect of HH momentum is low. Therefore, larger HF contribution (momentum) would increase the chances of the reaction being completed. The experiment has failed to show a specific trend which would also comply with the theory. The results at 2.9 and 3 violate Polanyi&#039;s rules as discussed in the previous question. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.1&amp;quot;&amp;gt;T. Bligaard, J.K. Nørskov, in Chemical Bonding at Surfaces and Interfaces, 2008&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.2&amp;quot;&amp;gt;Polanyi, J. C. Concepts in Reaction Dynamics Acc. Chem. Res. 1972, 5, 161– 168&amp;lt;/ref&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793680</id>
		<title>MRD:MToth96</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:MToth96&amp;diff=793680"/>
		<updated>2019-05-28T11:04:07Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /*  Q1 Potential Energy Surface */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Collision of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Potential Energy Surface&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
 [[File:Surface_Plot.PNG]]&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface (&#039;&#039;see above&#039;&#039;), the transition state is found and defined as the point where it is true that ∂V(ri)/∂ri=0, and ∂V2(ri)/∂ri2&amp;gt;0.                       &lt;br /&gt;
Empirically, the gradient of the surface is hence equals zero. Looking at the surface plot, the kinetic energy surface, as a function of AB distance has &lt;br /&gt;
a curvature that describes the potential energy as a function of distance. The transition state is at its minimum, as the distances are in balance. &lt;br /&gt;
Also, the trajectory (see black line) has to have its maximum value at the transition state, as we are expecting an energy maximum at this point. &lt;br /&gt;
The transition state is the highest point along the trajectory. At this point, AB and BC are also equal. After the second differentiation, a local maximum &lt;br /&gt;
is found if the derived value is positive. It is distinguished from other local minima by implementing the following criterium: ∂V/dq1 = 0 and ∂V/dq2 = 0, &lt;br /&gt;
where q1 is the tangent to the minimum and q2 is orthogonal to this as well as to the reaction path. Hence, ∂V2/dq12 &amp;lt; 0 and ∂V2/dq22 &amp;gt; 0 for that point.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This isn&#039;t quite correct. The transition state is both a maximum and a minimum, in different directions. In the direction of the minimum energy trajectory (i.e. the path the black line follows) it is a maximum. The second partial derivative of a maximum is always negative. Therefore the second partial derivative of the function of the PES in the direction of the reaction trajectory will be negative. However, as the TS occurs on the minimum energy pathway, this point is also a minimum, but in a direction orthogonal to the reaction trajectory. Therefore, as the second partial derivative of a minimum is always positive, the second partial derivative of the PES at the TS in the direction orthogonal to the trajectory will be positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 12:04, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Locating Transition States&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
When the transition state is reached, both the AB and BC distances are equal. Atoms show no vibration and therefore the graph displays no straight lines in accordance with this observation. The optimal distance was found to be 0.908 Å, at which both AB and BC distances were equal. Also, the momentum for both p1 and p2 were set to zero. &lt;br /&gt;
The Intermolecular distanced vs Time plot is shown below (on the left). The aim was to minimise oscillation and obtain flat lines with no corresponding gradients. No vibration means no change in distance and the vibration of the H atom and molecule is restricted. A restriction in vibrational freedom means that the TS is reached. Moreover, the BC and AB distances are equal and the corresponding lines are on top of each other. A static picture of the animation of the transition state can be seen below (on the right)&lt;br /&gt;
&lt;br /&gt;
[[File:Diastance_vs_time_h2.PNG]] .     [[File:Animation_h2_static.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 MEP and Dynamic Trajectory&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_mep.PNG]] .     [[File:Surface_dynamic.PNG]]&lt;br /&gt;
&lt;br /&gt;
The trajectory is displayed as the black line along the bottom of the surface plots (&#039;&#039;see above&#039;&#039;. When the MEP calculation (on the left) is used, the line starts from the transition state but is only displayed for a short length. Whereas, the dynamic calculation (on the right) gives a much longer, complete black trajectory. The program tries to find the steepest descent along the potential energy surface to obtained a minimum. The MEP method is being reset to zero after every step, whilst with dynamic calculation the data is being carried further to the next step. Hence, the calculation is being carried on regardless, whereas with MEP the kinetic energy stays at its minimum. Thus, an oscillating line with the dynamic, and a local maximum with the MEP calculation is being observed. &lt;br /&gt;
&lt;br /&gt;
[[File:normal.PNG]]               [[File:Changed_distance.PNG]]&lt;br /&gt;
&lt;br /&gt;
For comparison, values of interatomic distances were changed (&#039;&#039;see above&#039;&#039;. Values were being shifted from r1=ts+0.01, r2=ts (on the left); to r1=ts and r2=ts+0.01 (on the right)&lt;br /&gt;
In both cases, it was observed that the lines corresponding to the AB and BC distances were exchanged (as expected). When the numbers got changed, the transition state was approached by the opposite direction - as a symmetrical system is being considered - and the values are exactly the same but opposite. Hence, the same plot was displayed in the opposite direction. The same variations were applied for Momenta vs Time plots. The observations are exactly the same as for the distances, with the position of the lines being exchanged in between. The initial values are displayed below on the left, whereas the changed values can be seen on the right.&lt;br /&gt;
&lt;br /&gt;
[[File:Normal_momentum.PNG]]         [[File:Changed.PNG]]&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Reactivity through trajectory analysis &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; (kcal.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;
| -1.25 || -2.5  || -99.018 || Yes || A-B oscillates, B and C bond formation || [[File:-1.25,-2.5_p1,p2.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  || -100.456 || No || A-B oscillates, no reaction || [[File:-1.5,-2.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  || -98.956 || Yes || A-B oscillates, B and C bond formation || [[File:-1.5,-2.5.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  || -84.956 || No ||  A-B oscillates intensely, B and C bond formation is expected, but it bounces off and C remains a single atom || [[File:-2.5,-5.0.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  || -83.416 || Yes || 	A-B oscillates intensely, very close transition state, B and C bond formation || [[File:-2.5,-5.2.png]]&lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
From the table above it was concluded that the E total of the system depends on the momentum. Moreover, it shows a correlation with the kinetic energy of the system. The potential energy is constant and the kinetic energy is changing in response the structural changes. Furthermore, the system&#039;s susceptibility to undergo a reaction is also dependent on the momentum (not just on energy). If there is a large momentum difference between the single atom and the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule - especially when the incoming atom&#039;s momentum is marginally lower - than the reaction will not happen.&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5  Transition State Theory &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Transition State theory&amp;lt;ref name=&amp;quot;No.1&amp;quot; /&amp;gt; is a way of describing chemical reactions as such that the reaction consist of atoms and molecules are subjected to a continuous change in the energies and positions. The transition state is being described as the position along the reaction path where the energy is at its maximum. The activation energy corresponding to a specific reaction and to its reactant is the energy necessary to initiate collisions sufficient to reach the transition state. It is calculated as the difference between the reactants and the transition state. The transition state or activated complex is in equilibrium with the reactant and hence its properties can be approximated using Hammond&#039;s postulate. Moreover, the rate if reaction - formation of products - can be approximates from the concentration of these activated complexes and their ability to go to completion.&lt;br /&gt;
&lt;br /&gt;
Furthermore, the transition state theory can also be applied to the quasi-equilibrium state. The reactants are in equilibrium with the transition state complex. This means that an equilibrium is always established in between the reactant and the activated complex regardless of the relationship of the reactant and the product (if they are in equilibrium). This part of the theory can be materialised in the form of a mathematical expression through the Van Hoff equation. The equation describes an equilibrium state, which is reversible and temperature dependent. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{d\ln K}{dT} = \frac{\Delta U}{RT^{2}}&amp;lt;/math&amp;gt;    &#039;&#039;where, K - eq. constant, T - temperature in K, U - internal energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In order to get the temperature dependence of reaction rates, the equation is derived and as a result the Arrhenius equation is being formulated. The Arrhenius equation shows the temperature dependence of reaction rates as well as the activation energy of a corresponding reaction.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;k = Ae^{-E_a/RT}&amp;lt;/math&amp;gt;     &#039;&#039;where k - rate constant, T - temperature in K, A - exponential factor, Ea - activation energy, R - gas constant&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
According to the theory, the last reaction -  where P1 and P2 were -2.5 and -5.0 respectively - must go to completion. However, the exact opposite was observed. As a conclusion, it is suggested that the rate constant is lower in real life than it is in theory. Therefore, the rate constant prevents the reaction from going to completion. (the energy barrier is sufficient to retain AB as a molecule when is it being subjected to a collision by C)&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;System of F-H-H&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q1 Classification of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:FH_E_surface.png]]&lt;br /&gt;
&lt;br /&gt;
Atoms A and B are H-s, whereas C was F. The surface plot (&#039;&#039;see above&#039;&#039;) shows that the reactants (on the right hand side) are higher in energy than the product (on the left hand side). Therefore the reaction:&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H &lt;br /&gt;
&lt;br /&gt;
is exothermic (negative sign, accompanied by a decrease in energy). Hence the reverse reaction: &lt;br /&gt;
&lt;br /&gt;
H + HF → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F&lt;br /&gt;
&lt;br /&gt;
must be endothermic, as this is the corresponding backward reaction. In that case, the reactants will be lower in energy and the products will be higher. Additional energy is required to pass the activation energy barrier. &lt;br /&gt;
&lt;br /&gt;
[[File:HF_surfce_endothemic.png]] &lt;br /&gt;
&lt;br /&gt;
The first reaction is exothermic, (bond making is exothermic) which means that the final product will be in a lower energy state than the reactants. Hence, the HF bond is a stronger bond and is lower in energy than the H-H bond. This is due to the ionic nature of the H-F bond due to a large difference in electronegativity. The surface plot of the endothermic reaction is shown above. It can be depicted that the reactant are in a lower energy state than the product.&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q2 Position of the Transition State&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_plot_norxn.png]]      [[File:Contour_norxn.png]]&lt;br /&gt;
&lt;br /&gt;
To find the transition state, the surface (above, on the left) and contour (above, on the right) plots were displayed. At a transition state, only a single black dot can been seen on a surface plot as there is no trajectory. Moreover, the contour plot was left blank, as the reaction did not happen, but no oscillation is observed as the vibrational freedom of the complex is being retained. The transition state was obtained at H-H distance: 0.745 Å, and H-F distance: 1.808 Å.&lt;br /&gt;
&lt;br /&gt;
For these calculations p1=p2=0 &lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q3 Activation Energies &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Using the Energy vs Time plots, the following values have been established:&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F → HF + H:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -103.913 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 0.226 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F:&lt;br /&gt;
&lt;br /&gt;
Transition state: -103.687 kcal.mol-1&lt;br /&gt;
Reactants: -132.455 kcal.mol-1&lt;br /&gt;
Activation energy (difference): 28.768 kcal.mol-1&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q4 Mechanisms of energy release&amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
A scenario was set up in which the Animation and Momenta vs Time plots show that the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; - F reaction goes to completion. B and C were the H and A was the F atoms, with distances of A-B 1.5 Å, and B-C 0.878 Å. &lt;br /&gt;
&lt;br /&gt;
[[File:mom_vs_time_AB_1.5_BC_0.878.png]]&lt;br /&gt;
&lt;br /&gt;
When the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule collides with the F atom, the translational energy of the species (due to the attraction between them) is being transformed into vibrational energy (oscillation being observed). Depending on the nature of the experiment, exothermic reactions release whereas, endothermic reactions absorb energy (in the form of heat) from the environment. When the oscillating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (both) atom approaches the  F atom (only translational energy), oscillation in the form of vibrational energy is being transmitted to the residual HF molecule. This way, the energy of the system is constant but the vibrational and kinetic energies are being transformed in between species. This can be confirmed experimentally by measuring the vibrational energy of the system via IR spectroscopy or use bomb calorimetry to determine the kinetic energy of the system  - which is directly proportional to the translational energy and its momentum. &lt;br /&gt;
&lt;br /&gt;
rHH = 0.74 Å, with a momentum pFH = -0.5, pHH in the range -3 to 3, rHF was set to 1.5 Å&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! pHH !! Level of Vibration of H-H bond !! Reaction &lt;br /&gt;
|-&lt;br /&gt;
| -3 || medium || transition state &lt;br /&gt;
|-&lt;br /&gt;
| -2.9 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.8 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.7 || medium || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| -2.6 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -2.25 || medium || no &lt;br /&gt;
|-&lt;br /&gt;
|  -2|| medium || no &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| -1 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 0 || strong|| yes &lt;br /&gt;
|-&lt;br /&gt;
| 1 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 1.5 || weak || transition state &lt;br /&gt;
|-&lt;br /&gt;
|  2 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.25  || medium || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.3 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.4 || weak || no &lt;br /&gt;
|-&lt;br /&gt;
| 2.5 || medium || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.6 || weak || yes &lt;br /&gt;
|-&lt;br /&gt;
| 2.7 ||  weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
|  2.8 || weak || transition state  &lt;br /&gt;
|-&lt;br /&gt;
| 2.9  || weak || yes  &lt;br /&gt;
|-&lt;br /&gt;
| 3 || medium || yes &lt;br /&gt;
|}&lt;br /&gt;
&#039;&#039;&#039;(Table 1)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction goes to completion between the values -1.5 and 1, 2.5-2.6 and 2.9-3.0. As a conclusion, it was determined that no certain trends can be depicted from the data which would link the momentum, the outcome and the stretch of vibrations together. Moreover, the reactions at 2.9 and 3.0 are against Polanyi&#039;s empirical rule.&lt;br /&gt;
&lt;br /&gt;
For a separate calculation, the same initial positions were used, for HF + H → H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F  with rHH=0.74 A but the momentum of HF was changed to p= -0.8 and the HH momentum was 0.1. The reaction goes to completion and thus the reaction is valid!&lt;br /&gt;
&lt;br /&gt;
If we look at the Momenta vs Time plot, we can see a continuously oscillating path, hence the reaction had reached its end. A large momentum contribution is seen as a a result of a large contribution from the very strong HF bond. &lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; 2 Å&lt;br /&gt;
HF 0.893325 Å&lt;br /&gt;
Phh - 8&lt;br /&gt;
Phf -0,02&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;u&amp;gt; Q5 Polanyi&#039;s Empirical Rule and the Distribution of Energy &amp;lt;/u&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
Polany&#039;s empirical rules&amp;lt;ref name=&amp;quot;No.2&amp;quot; /&amp;gt; are reflecting on the effect of transition states energetically different modes. An exothermic reaction - in which the products are higher in energy - the transition state is described as &#039;early&#039; as it is closer in energy to the reactants. Hence, the translational energy has a greater impact on the activated complex snd thus the reaction then the vibrational energy. Empirically, for an endothermic reaction -  with a corresponding late transition state - the vibrational energy has a greater importance on the reaction.&lt;br /&gt;
&lt;br /&gt;
In this case, &lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → HF + H&lt;br /&gt;
&lt;br /&gt;
is an exothermic reaction. Therefore, as described above it has an early transition state which suggest a greater impact from the translational energy contribution. The vibrational energy can be seen through the oscillating nature of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule, where the translational contribution is largely coming from the H-F bond (both can be seen through their momenta). The effect of HH momentum is low. Therefore, larger HF contribution (momentum) would increase the chances of the reaction being completed. The experiment has failed to show a specific trend which would also comply with the theory. The results at 2.9 and 3 violate Polanyi&#039;s rules as discussed in the previous question. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.1&amp;quot;&amp;gt;T. Bligaard, J.K. Nørskov, in Chemical Bonding at Surfaces and Interfaces, 2008&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;No.2&amp;quot;&amp;gt;Polanyi, J. C. Concepts in Reaction Dynamics Acc. Chem. Res. 1972, 5, 161– 168&amp;lt;/ref&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793679</id>
		<title>MRD:ql2817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793679"/>
		<updated>2019-05-28T10:53:16Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* 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;&lt;br /&gt;
== &#039;&#039;&#039;Question 1&#039;&#039;&#039; ==&lt;br /&gt;
&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;
&lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.It is located at the saddle point in the potential energy surface diagram, which defined as : ∂V(ri)/∂ri=0 and H &amp;lt; 0, where H = frr(r0​,V0​)fVV(r0​,V0​)−f2rV​(r0​,V0​) .&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|The first sentence is correct however your mathematical definition isn&#039;t very clear. Because the TS is a maximum in one direction, the second partial derivative of that function with respect to the TS will be negative, as the second partial derivative of a maximum is always negative. However, it is the maximum on the trajectory of the minimum energy pathway and therefore in the direction that is orthogonal to the reaction trajectory, it is a minimum (in the direction of a cross-section of the well of the pathway) and therefore the second partial derivative will be positive as a second partial derivative of a minimum is always positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The transition state is the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Really not sure what this means, sorry! [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== 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;
When r(AB)=r(BC)=0.907 Å, p1 = p2 = 0.0, the transition state occurs. The internuclear distance vs time graph gives a relatively straight line which indicates a constant distance.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| And why would a &amp;quot;constant distance&amp;quot; (of what exactly - be explicit and specific) mean that you are at the TS? Make sure you always explain your answers thoroughly in order to demonstrate your understanding of the depths of the theory. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:44, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the mep and the trajectory you just calculated differ. ===&lt;br /&gt;
The mep trajectory keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Exactly, but why? What does it mean, in terms of energy, momenta and the calculations themselves? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:48, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
r1 = 0.907, r2 = 0.917&lt;br /&gt;
&lt;br /&gt;
Molecules and atome moving away from each other.&lt;br /&gt;
&lt;br /&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;
&lt;br /&gt;
r1 = rts+δ, r2 = rts&lt;br /&gt;
&lt;br /&gt;
final values of the positions r1(t) = 3.45, r2(t) = 0.72 and the average momenta  p1(t) = -1.45, p2(t) = -2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
The molecule and the atom moving close together instead of moving apart.&lt;br /&gt;
&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; border=&amp;quot;5&amp;quot;&lt;br /&gt;
! P1!!P2 !! Etot!! Reactive?!!Description of the dyanmics!!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5|| -99.08|| yes||The trajectory goes through the transition state and also go into the products. ||[[File:Surface01_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5|| -2.0|| -100.22|| no||The trajectory falls back down into the reactants because there was not enough energy for reactants to pass over the transition state. || [[File:Surface02_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5||  -2.5|| -98.91|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface03_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5|| -5.0|| -84.62|| no||The trajectory was carrying enough energy towards products but then it shifts back into the reactants. || [[File:Surface04_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5||  -5.2|| -83.40|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface05_ql2817.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|So what can you conclude from these observations? Is the trend in total energy enough to dictate whether or not a reaction will be successful? (It&#039;s not, but why?) [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:50, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;main&amp;quot;&amp;gt;https://en.wikibooks.org/wiki/Statistical_Thermodynamics_and_Rate_Theories/Eyring_Transition_State_Theory#Assumptions_of_Transition_State_Theory&lt;br /&gt;
&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
*Reactants are in constant equilibrium with the transition state structure.&lt;br /&gt;
*The energy of the particles follow a Boltzmann distribution.&lt;br /&gt;
*Once reactants become the transition state, the transition state structure does not collapse back to the reactants.&lt;br /&gt;
&lt;br /&gt;
Transition state theory will predict a higher reaction rate than experimental one.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This is all correct, but why? Which of these 3 points is untrue and how does it not reflect real life reactions, and why does this mean that the rate will be overpredicted? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:50, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;Exercise 2: F-H-H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
===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;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-01.png]]&lt;br /&gt;
&lt;br /&gt;
exothermic, because the trajectory goes from a higher PE to a lower PE.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+F2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-02.png]]&lt;br /&gt;
&lt;br /&gt;
endothermic, because the trajectory goes from a lower PE to a higher PE.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|You haven&#039;t commented on the relative bond strengths of the species involved. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:50, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 1.8108&lt;br /&gt;
r(BC): 0.744877&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-03.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+HF:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 0.744877&lt;br /&gt;
r(BC): 1.8108&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-04.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 30 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-05.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+FH::&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 0.44kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-06.png]]&lt;br /&gt;
&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;
reactive trajectory:&lt;br /&gt;
&lt;br /&gt;
r(AB):1.6, r(BC):0.74, P AB:-0.5, P BC:0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-07.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-08.png]]&lt;br /&gt;
&lt;br /&gt;
From the graph above, it is clearly shown that total energy remains the same. Kinetic energy increases to the same extent as potential energy decreases.&lt;br /&gt;
This proves that energy is conserved. This can be confirmed experimentally by measuring the kinetic and potential energy in the real experiment, ie measure temperature change and potential energy can be measured using this software.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Can  you highlight a particular experiment that could do this? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:51, 28 May 2019 (BST)}}&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;
[[File:ql2817-09.png]]&lt;br /&gt;
&lt;br /&gt;
high translational energy, r(AB)=2, r(BC)=0.74, P AB=-7, P BC=0.5&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-10.png]]&lt;br /&gt;
&lt;br /&gt;
high vibrational energy, r(AB)=2, r(BC)=0.74, P AB=-1, P BC=6&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The reaction is a late TS reaction, also Polanyi&#039;s empirical rules tells us that vibrational energy is more important in compare to vibrational energy in a late transition state reaction, which can also be proved in the graphs above.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This answer is not sufficient to demonstrate what the question asks. You need to be a bit more thorough i.e. explain Polanyi&#039;s rules more clearly and in more detail, and use several examples to demostrate the rules in reactions. You also need to annotate diagrams with explanations that discuss exactly how that proves Polanyi&#039;s rules. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:53, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
==&#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&amp;lt;references/&amp;gt;:&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793678</id>
		<title>MRD:ql2817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793678"/>
		<updated>2019-05-28T10:51:40Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* 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;&lt;br /&gt;
== &#039;&#039;&#039;Question 1&#039;&#039;&#039; ==&lt;br /&gt;
&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;
&lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.It is located at the saddle point in the potential energy surface diagram, which defined as : ∂V(ri)/∂ri=0 and H &amp;lt; 0, where H = frr(r0​,V0​)fVV(r0​,V0​)−f2rV​(r0​,V0​) .&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|The first sentence is correct however your mathematical definition isn&#039;t very clear. Because the TS is a maximum in one direction, the second partial derivative of that function with respect to the TS will be negative, as the second partial derivative of a maximum is always negative. However, it is the maximum on the trajectory of the minimum energy pathway and therefore in the direction that is orthogonal to the reaction trajectory, it is a minimum (in the direction of a cross-section of the well of the pathway) and therefore the second partial derivative will be positive as a second partial derivative of a minimum is always positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The transition state is the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Really not sure what this means, sorry! [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== 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;
When r(AB)=r(BC)=0.907 Å, p1 = p2 = 0.0, the transition state occurs. The internuclear distance vs time graph gives a relatively straight line which indicates a constant distance.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| And why would a &amp;quot;constant distance&amp;quot; (of what exactly - be explicit and specific) mean that you are at the TS? Make sure you always explain your answers thoroughly in order to demonstrate your understanding of the depths of the theory. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:44, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the mep and the trajectory you just calculated differ. ===&lt;br /&gt;
The mep trajectory keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Exactly, but why? What does it mean, in terms of energy, momenta and the calculations themselves? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:48, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
r1 = 0.907, r2 = 0.917&lt;br /&gt;
&lt;br /&gt;
Molecules and atome moving away from each other.&lt;br /&gt;
&lt;br /&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;
&lt;br /&gt;
r1 = rts+δ, r2 = rts&lt;br /&gt;
&lt;br /&gt;
final values of the positions r1(t) = 3.45, r2(t) = 0.72 and the average momenta  p1(t) = -1.45, p2(t) = -2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
The molecule and the atom moving close together instead of moving apart.&lt;br /&gt;
&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; border=&amp;quot;5&amp;quot;&lt;br /&gt;
! P1!!P2 !! Etot!! Reactive?!!Description of the dyanmics!!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5|| -99.08|| yes||The trajectory goes through the transition state and also go into the products. ||[[File:Surface01_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5|| -2.0|| -100.22|| no||The trajectory falls back down into the reactants because there was not enough energy for reactants to pass over the transition state. || [[File:Surface02_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5||  -2.5|| -98.91|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface03_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5|| -5.0|| -84.62|| no||The trajectory was carrying enough energy towards products but then it shifts back into the reactants. || [[File:Surface04_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5||  -5.2|| -83.40|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface05_ql2817.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|So what can you conclude from these observations? Is the trend in total energy enough to dictate whether or not a reaction will be successful? (It&#039;s not, but why?) [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:50, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;main&amp;quot;&amp;gt;https://en.wikibooks.org/wiki/Statistical_Thermodynamics_and_Rate_Theories/Eyring_Transition_State_Theory#Assumptions_of_Transition_State_Theory&lt;br /&gt;
&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
*Reactants are in constant equilibrium with the transition state structure.&lt;br /&gt;
*The energy of the particles follow a Boltzmann distribution.&lt;br /&gt;
*Once reactants become the transition state, the transition state structure does not collapse back to the reactants.&lt;br /&gt;
&lt;br /&gt;
Transition state theory will predict a higher reaction rate than experimental one.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This is all correct, but why? Which of these 3 points is untrue and how does it not reflect real life reactions, and why does this mean that the rate will be overpredicted? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:50, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;Exercise 2: F-H-H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
===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;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-01.png]]&lt;br /&gt;
&lt;br /&gt;
exothermic, because the trajectory goes from a higher PE to a lower PE.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+F2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-02.png]]&lt;br /&gt;
&lt;br /&gt;
endothermic, because the trajectory goes from a lower PE to a higher PE.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|You haven&#039;t commented on the relative bond strengths of the species involved. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:50, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 1.8108&lt;br /&gt;
r(BC): 0.744877&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-03.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+HF:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 0.744877&lt;br /&gt;
r(BC): 1.8108&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-04.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 30 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-05.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+FH::&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 0.44kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-06.png]]&lt;br /&gt;
&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;
reactive trajectory:&lt;br /&gt;
&lt;br /&gt;
r(AB):1.6, r(BC):0.74, P AB:-0.5, P BC:0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-07.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-08.png]]&lt;br /&gt;
&lt;br /&gt;
From the graph above, it is clearly shown that total energy remains the same. Kinetic energy increases to the same extent as potential energy decreases.&lt;br /&gt;
This proves that energy is conserved. This can be confirmed experimentally by measuring the kinetic and potential energy in the real experiment, ie measure temperature change and potential energy can be measured using this software.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Can  you highlight a particular experiment that could do this? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:51, 28 May 2019 (BST)}}&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;
[[File:ql2817-09.png]]&lt;br /&gt;
&lt;br /&gt;
high translational energy, r(AB)=2, r(BC)=0.74, P AB=-7, P BC=0.5&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-10.png]]&lt;br /&gt;
&lt;br /&gt;
high vibrational energy, r(AB)=2, r(BC)=0.74, P AB=-1, P BC=6&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The reaction is a late TS reaction, also Polanyi&#039;s empirical rules tells us that vibrational energy is more important in compare to vibrational energy in a late transition state reaction, which can also be proved in the graphs above.&lt;br /&gt;
&lt;br /&gt;
==&#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&amp;lt;references/&amp;gt;:&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793677</id>
		<title>MRD:ql2817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793677"/>
		<updated>2019-05-28T10:50:46Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* 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;&lt;br /&gt;
== &#039;&#039;&#039;Question 1&#039;&#039;&#039; ==&lt;br /&gt;
&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;
&lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.It is located at the saddle point in the potential energy surface diagram, which defined as : ∂V(ri)/∂ri=0 and H &amp;lt; 0, where H = frr(r0​,V0​)fVV(r0​,V0​)−f2rV​(r0​,V0​) .&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|The first sentence is correct however your mathematical definition isn&#039;t very clear. Because the TS is a maximum in one direction, the second partial derivative of that function with respect to the TS will be negative, as the second partial derivative of a maximum is always negative. However, it is the maximum on the trajectory of the minimum energy pathway and therefore in the direction that is orthogonal to the reaction trajectory, it is a minimum (in the direction of a cross-section of the well of the pathway) and therefore the second partial derivative will be positive as a second partial derivative of a minimum is always positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The transition state is the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Really not sure what this means, sorry! [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== 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;
When r(AB)=r(BC)=0.907 Å, p1 = p2 = 0.0, the transition state occurs. The internuclear distance vs time graph gives a relatively straight line which indicates a constant distance.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| And why would a &amp;quot;constant distance&amp;quot; (of what exactly - be explicit and specific) mean that you are at the TS? Make sure you always explain your answers thoroughly in order to demonstrate your understanding of the depths of the theory. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:44, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the mep and the trajectory you just calculated differ. ===&lt;br /&gt;
The mep trajectory keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Exactly, but why? What does it mean, in terms of energy, momenta and the calculations themselves? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:48, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
r1 = 0.907, r2 = 0.917&lt;br /&gt;
&lt;br /&gt;
Molecules and atome moving away from each other.&lt;br /&gt;
&lt;br /&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;
&lt;br /&gt;
r1 = rts+δ, r2 = rts&lt;br /&gt;
&lt;br /&gt;
final values of the positions r1(t) = 3.45, r2(t) = 0.72 and the average momenta  p1(t) = -1.45, p2(t) = -2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
The molecule and the atom moving close together instead of moving apart.&lt;br /&gt;
&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; border=&amp;quot;5&amp;quot;&lt;br /&gt;
! P1!!P2 !! Etot!! Reactive?!!Description of the dyanmics!!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5|| -99.08|| yes||The trajectory goes through the transition state and also go into the products. ||[[File:Surface01_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5|| -2.0|| -100.22|| no||The trajectory falls back down into the reactants because there was not enough energy for reactants to pass over the transition state. || [[File:Surface02_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5||  -2.5|| -98.91|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface03_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5|| -5.0|| -84.62|| no||The trajectory was carrying enough energy towards products but then it shifts back into the reactants. || [[File:Surface04_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5||  -5.2|| -83.40|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface05_ql2817.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|So what can you conclude from these observations? Is the trend in total energy enough to dictate whether or not a reaction will be successful? (It&#039;s not, but why?) [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:50, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;main&amp;quot;&amp;gt;https://en.wikibooks.org/wiki/Statistical_Thermodynamics_and_Rate_Theories/Eyring_Transition_State_Theory#Assumptions_of_Transition_State_Theory&lt;br /&gt;
&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
*Reactants are in constant equilibrium with the transition state structure.&lt;br /&gt;
*The energy of the particles follow a Boltzmann distribution.&lt;br /&gt;
*Once reactants become the transition state, the transition state structure does not collapse back to the reactants.&lt;br /&gt;
&lt;br /&gt;
Transition state theory will predict a higher reaction rate than experimental one.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This is all correct, but why? Which of these 3 points is untrue and how does it not reflect real life reactions, and why does this mean that the rate will be overpredicted? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:50, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;Exercise 2: F-H-H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
===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;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-01.png]]&lt;br /&gt;
&lt;br /&gt;
exothermic, because the trajectory goes from a higher PE to a lower PE.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+F2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-02.png]]&lt;br /&gt;
&lt;br /&gt;
endothermic, because the trajectory goes from a lower PE to a higher PE.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|You haven&#039;t commented on the relative bond strengths of the species involved. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:50, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 1.8108&lt;br /&gt;
r(BC): 0.744877&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-03.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+HF:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 0.744877&lt;br /&gt;
r(BC): 1.8108&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-04.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 30 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-05.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+FH::&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 0.44kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-06.png]]&lt;br /&gt;
&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;
reactive trajectory:&lt;br /&gt;
&lt;br /&gt;
r(AB):1.6, r(BC):0.74, P AB:-0.5, P BC:0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-07.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-08.png]]&lt;br /&gt;
&lt;br /&gt;
From the graph above, it is clearly shown that total energy remains the same. Kinetic energy increases to the same extent as potential energy decreases.&lt;br /&gt;
This proves that energy is conserved. This can be confirmed experimentally by measuring the kinetic and potential energy in the real experiment, ie measure temperature change and potential energy can be measured using this software.&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;
[[File:ql2817-09.png]]&lt;br /&gt;
&lt;br /&gt;
high translational energy, r(AB)=2, r(BC)=0.74, P AB=-7, P BC=0.5&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-10.png]]&lt;br /&gt;
&lt;br /&gt;
high vibrational energy, r(AB)=2, r(BC)=0.74, P AB=-1, P BC=6&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The reaction is a late TS reaction, also Polanyi&#039;s empirical rules tells us that vibrational energy is more important in compare to vibrational energy in a late transition state reaction, which can also be proved in the graphs above.&lt;br /&gt;
&lt;br /&gt;
==&#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&amp;lt;references/&amp;gt;:&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793676</id>
		<title>MRD:ql2817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793676"/>
		<updated>2019-05-28T10:50:13Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* State what are the main assumptions of Transition State Theory. 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;&lt;br /&gt;
== &#039;&#039;&#039;Question 1&#039;&#039;&#039; ==&lt;br /&gt;
&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;
&lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.It is located at the saddle point in the potential energy surface diagram, which defined as : ∂V(ri)/∂ri=0 and H &amp;lt; 0, where H = frr(r0​,V0​)fVV(r0​,V0​)−f2rV​(r0​,V0​) .&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|The first sentence is correct however your mathematical definition isn&#039;t very clear. Because the TS is a maximum in one direction, the second partial derivative of that function with respect to the TS will be negative, as the second partial derivative of a maximum is always negative. However, it is the maximum on the trajectory of the minimum energy pathway and therefore in the direction that is orthogonal to the reaction trajectory, it is a minimum (in the direction of a cross-section of the well of the pathway) and therefore the second partial derivative will be positive as a second partial derivative of a minimum is always positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The transition state is the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Really not sure what this means, sorry! [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== 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;
When r(AB)=r(BC)=0.907 Å, p1 = p2 = 0.0, the transition state occurs. The internuclear distance vs time graph gives a relatively straight line which indicates a constant distance.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| And why would a &amp;quot;constant distance&amp;quot; (of what exactly - be explicit and specific) mean that you are at the TS? Make sure you always explain your answers thoroughly in order to demonstrate your understanding of the depths of the theory. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:44, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the mep and the trajectory you just calculated differ. ===&lt;br /&gt;
The mep trajectory keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Exactly, but why? What does it mean, in terms of energy, momenta and the calculations themselves? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:48, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
r1 = 0.907, r2 = 0.917&lt;br /&gt;
&lt;br /&gt;
Molecules and atome moving away from each other.&lt;br /&gt;
&lt;br /&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;
&lt;br /&gt;
r1 = rts+δ, r2 = rts&lt;br /&gt;
&lt;br /&gt;
final values of the positions r1(t) = 3.45, r2(t) = 0.72 and the average momenta  p1(t) = -1.45, p2(t) = -2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
The molecule and the atom moving close together instead of moving apart.&lt;br /&gt;
&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; border=&amp;quot;5&amp;quot;&lt;br /&gt;
! P1!!P2 !! Etot!! Reactive?!!Description of the dyanmics!!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5|| -99.08|| yes||The trajectory goes through the transition state and also go into the products. ||[[File:Surface01_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5|| -2.0|| -100.22|| no||The trajectory falls back down into the reactants because there was not enough energy for reactants to pass over the transition state. || [[File:Surface02_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5||  -2.5|| -98.91|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface03_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5|| -5.0|| -84.62|| no||The trajectory was carrying enough energy towards products but then it shifts back into the reactants. || [[File:Surface04_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5||  -5.2|| -83.40|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface05_ql2817.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|So what can you conclude from these observations? Is the trend in total energy enough to dictate whether or not a reaction will be successful? (It&#039;s not, but why?) [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:50, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;main&amp;quot;&amp;gt;https://en.wikibooks.org/wiki/Statistical_Thermodynamics_and_Rate_Theories/Eyring_Transition_State_Theory#Assumptions_of_Transition_State_Theory&lt;br /&gt;
&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
*Reactants are in constant equilibrium with the transition state structure.&lt;br /&gt;
*The energy of the particles follow a Boltzmann distribution.&lt;br /&gt;
*Once reactants become the transition state, the transition state structure does not collapse back to the reactants.&lt;br /&gt;
&lt;br /&gt;
Transition state theory will predict a higher reaction rate than experimental one.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This is all correct, but why? Which of these 3 points is untrue and how does it not reflect real life reactions, and why does this mean that the rate will be overpredicted? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:50, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;Exercise 2: F-H-H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
===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;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-01.png]]&lt;br /&gt;
&lt;br /&gt;
exothermic, because the trajectory goes from a higher PE to a lower PE.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+F2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-02.png]]&lt;br /&gt;
&lt;br /&gt;
endothermic, because the trajectory goes from a lower PE to a higher PE.&lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 1.8108&lt;br /&gt;
r(BC): 0.744877&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-03.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+HF:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 0.744877&lt;br /&gt;
r(BC): 1.8108&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-04.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 30 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-05.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+FH::&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 0.44kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-06.png]]&lt;br /&gt;
&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;
reactive trajectory:&lt;br /&gt;
&lt;br /&gt;
r(AB):1.6, r(BC):0.74, P AB:-0.5, P BC:0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-07.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-08.png]]&lt;br /&gt;
&lt;br /&gt;
From the graph above, it is clearly shown that total energy remains the same. Kinetic energy increases to the same extent as potential energy decreases.&lt;br /&gt;
This proves that energy is conserved. This can be confirmed experimentally by measuring the kinetic and potential energy in the real experiment, ie measure temperature change and potential energy can be measured using this software.&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;
[[File:ql2817-09.png]]&lt;br /&gt;
&lt;br /&gt;
high translational energy, r(AB)=2, r(BC)=0.74, P AB=-7, P BC=0.5&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-10.png]]&lt;br /&gt;
&lt;br /&gt;
high vibrational energy, r(AB)=2, r(BC)=0.74, P AB=-1, P BC=6&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The reaction is a late TS reaction, also Polanyi&#039;s empirical rules tells us that vibrational energy is more important in compare to vibrational energy in a late transition state reaction, which can also be proved in the graphs above.&lt;br /&gt;
&lt;br /&gt;
==&#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&amp;lt;references/&amp;gt;:&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793675</id>
		<title>MRD:ql2817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793675"/>
		<updated>2019-05-28T10:48:21Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Comment on how the mep and the trajectory you just calculated differ. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;Question 1&#039;&#039;&#039; ==&lt;br /&gt;
&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;
&lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.It is located at the saddle point in the potential energy surface diagram, which defined as : ∂V(ri)/∂ri=0 and H &amp;lt; 0, where H = frr(r0​,V0​)fVV(r0​,V0​)−f2rV​(r0​,V0​) .&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|The first sentence is correct however your mathematical definition isn&#039;t very clear. Because the TS is a maximum in one direction, the second partial derivative of that function with respect to the TS will be negative, as the second partial derivative of a maximum is always negative. However, it is the maximum on the trajectory of the minimum energy pathway and therefore in the direction that is orthogonal to the reaction trajectory, it is a minimum (in the direction of a cross-section of the well of the pathway) and therefore the second partial derivative will be positive as a second partial derivative of a minimum is always positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The transition state is the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Really not sure what this means, sorry! [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== 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;
When r(AB)=r(BC)=0.907 Å, p1 = p2 = 0.0, the transition state occurs. The internuclear distance vs time graph gives a relatively straight line which indicates a constant distance.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| And why would a &amp;quot;constant distance&amp;quot; (of what exactly - be explicit and specific) mean that you are at the TS? Make sure you always explain your answers thoroughly in order to demonstrate your understanding of the depths of the theory. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:44, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the mep and the trajectory you just calculated differ. ===&lt;br /&gt;
The mep trajectory keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Exactly, but why? What does it mean, in terms of energy, momenta and the calculations themselves? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:48, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
r1 = 0.907, r2 = 0.917&lt;br /&gt;
&lt;br /&gt;
Molecules and atome moving away from each other.&lt;br /&gt;
&lt;br /&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;
&lt;br /&gt;
r1 = rts+δ, r2 = rts&lt;br /&gt;
&lt;br /&gt;
final values of the positions r1(t) = 3.45, r2(t) = 0.72 and the average momenta  p1(t) = -1.45, p2(t) = -2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
The molecule and the atom moving close together instead of moving apart.&lt;br /&gt;
&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; border=&amp;quot;5&amp;quot;&lt;br /&gt;
! P1!!P2 !! Etot!! Reactive?!!Description of the dyanmics!!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5|| -99.08|| yes||The trajectory goes through the transition state and also go into the products. ||[[File:Surface01_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5|| -2.0|| -100.22|| no||The trajectory falls back down into the reactants because there was not enough energy for reactants to pass over the transition state. || [[File:Surface02_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5||  -2.5|| -98.91|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface03_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5|| -5.0|| -84.62|| no||The trajectory was carrying enough energy towards products but then it shifts back into the reactants. || [[File:Surface04_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5||  -5.2|| -83.40|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface05_ql2817.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;main&amp;quot;&amp;gt;https://en.wikibooks.org/wiki/Statistical_Thermodynamics_and_Rate_Theories/Eyring_Transition_State_Theory#Assumptions_of_Transition_State_Theory&lt;br /&gt;
&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
*Reactants are in constant equilibrium with the transition state structure.&lt;br /&gt;
*The energy of the particles follow a Boltzmann distribution.&lt;br /&gt;
*Once reactants become the transition state, the transition state structure does not collapse back to the reactants.&lt;br /&gt;
&lt;br /&gt;
Transition state theory will predict a higher reaction rate than experimental one.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;Exercise 2: F-H-H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
===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;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-01.png]]&lt;br /&gt;
&lt;br /&gt;
exothermic, because the trajectory goes from a higher PE to a lower PE.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+F2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-02.png]]&lt;br /&gt;
&lt;br /&gt;
endothermic, because the trajectory goes from a lower PE to a higher PE.&lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 1.8108&lt;br /&gt;
r(BC): 0.744877&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-03.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+HF:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 0.744877&lt;br /&gt;
r(BC): 1.8108&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-04.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 30 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-05.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+FH::&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 0.44kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-06.png]]&lt;br /&gt;
&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;
reactive trajectory:&lt;br /&gt;
&lt;br /&gt;
r(AB):1.6, r(BC):0.74, P AB:-0.5, P BC:0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-07.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-08.png]]&lt;br /&gt;
&lt;br /&gt;
From the graph above, it is clearly shown that total energy remains the same. Kinetic energy increases to the same extent as potential energy decreases.&lt;br /&gt;
This proves that energy is conserved. This can be confirmed experimentally by measuring the kinetic and potential energy in the real experiment, ie measure temperature change and potential energy can be measured using this software.&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;
[[File:ql2817-09.png]]&lt;br /&gt;
&lt;br /&gt;
high translational energy, r(AB)=2, r(BC)=0.74, P AB=-7, P BC=0.5&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-10.png]]&lt;br /&gt;
&lt;br /&gt;
high vibrational energy, r(AB)=2, r(BC)=0.74, P AB=-1, P BC=6&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The reaction is a late TS reaction, also Polanyi&#039;s empirical rules tells us that vibrational energy is more important in compare to vibrational energy in a late transition state reaction, which can also be proved in the graphs above.&lt;br /&gt;
&lt;br /&gt;
==&#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&amp;lt;references/&amp;gt;:&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793674</id>
		<title>MRD:ql2817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793674"/>
		<updated>2019-05-28T10:44:07Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* 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;&lt;br /&gt;
== &#039;&#039;&#039;Question 1&#039;&#039;&#039; ==&lt;br /&gt;
&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;
&lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.It is located at the saddle point in the potential energy surface diagram, which defined as : ∂V(ri)/∂ri=0 and H &amp;lt; 0, where H = frr(r0​,V0​)fVV(r0​,V0​)−f2rV​(r0​,V0​) .&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|The first sentence is correct however your mathematical definition isn&#039;t very clear. Because the TS is a maximum in one direction, the second partial derivative of that function with respect to the TS will be negative, as the second partial derivative of a maximum is always negative. However, it is the maximum on the trajectory of the minimum energy pathway and therefore in the direction that is orthogonal to the reaction trajectory, it is a minimum (in the direction of a cross-section of the well of the pathway) and therefore the second partial derivative will be positive as a second partial derivative of a minimum is always positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The transition state is the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Really not sure what this means, sorry! [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== 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;
When r(AB)=r(BC)=0.907 Å, p1 = p2 = 0.0, the transition state occurs. The internuclear distance vs time graph gives a relatively straight line which indicates a constant distance.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| And why would a &amp;quot;constant distance&amp;quot; (of what exactly - be explicit and specific) mean that you are at the TS? Make sure you always explain your answers thoroughly in order to demonstrate your understanding of the depths of the theory. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:44, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the mep and the trajectory you just calculated differ. ===&lt;br /&gt;
The mep trajectory keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy.&lt;br /&gt;
&lt;br /&gt;
r1 = 0.907, r2 = 0.917&lt;br /&gt;
&lt;br /&gt;
Molecules and atome moving away from each other.&lt;br /&gt;
&lt;br /&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;
&lt;br /&gt;
r1 = rts+δ, r2 = rts&lt;br /&gt;
&lt;br /&gt;
final values of the positions r1(t) = 3.45, r2(t) = 0.72 and the average momenta  p1(t) = -1.45, p2(t) = -2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
The molecule and the atom moving close together instead of moving apart.&lt;br /&gt;
&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; border=&amp;quot;5&amp;quot;&lt;br /&gt;
! P1!!P2 !! Etot!! Reactive?!!Description of the dyanmics!!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5|| -99.08|| yes||The trajectory goes through the transition state and also go into the products. ||[[File:Surface01_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5|| -2.0|| -100.22|| no||The trajectory falls back down into the reactants because there was not enough energy for reactants to pass over the transition state. || [[File:Surface02_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5||  -2.5|| -98.91|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface03_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5|| -5.0|| -84.62|| no||The trajectory was carrying enough energy towards products but then it shifts back into the reactants. || [[File:Surface04_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5||  -5.2|| -83.40|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface05_ql2817.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;main&amp;quot;&amp;gt;https://en.wikibooks.org/wiki/Statistical_Thermodynamics_and_Rate_Theories/Eyring_Transition_State_Theory#Assumptions_of_Transition_State_Theory&lt;br /&gt;
&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
*Reactants are in constant equilibrium with the transition state structure.&lt;br /&gt;
*The energy of the particles follow a Boltzmann distribution.&lt;br /&gt;
*Once reactants become the transition state, the transition state structure does not collapse back to the reactants.&lt;br /&gt;
&lt;br /&gt;
Transition state theory will predict a higher reaction rate than experimental one.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;Exercise 2: F-H-H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
===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;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-01.png]]&lt;br /&gt;
&lt;br /&gt;
exothermic, because the trajectory goes from a higher PE to a lower PE.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+F2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-02.png]]&lt;br /&gt;
&lt;br /&gt;
endothermic, because the trajectory goes from a lower PE to a higher PE.&lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 1.8108&lt;br /&gt;
r(BC): 0.744877&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-03.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+HF:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 0.744877&lt;br /&gt;
r(BC): 1.8108&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-04.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 30 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-05.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+FH::&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 0.44kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-06.png]]&lt;br /&gt;
&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;
reactive trajectory:&lt;br /&gt;
&lt;br /&gt;
r(AB):1.6, r(BC):0.74, P AB:-0.5, P BC:0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-07.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-08.png]]&lt;br /&gt;
&lt;br /&gt;
From the graph above, it is clearly shown that total energy remains the same. Kinetic energy increases to the same extent as potential energy decreases.&lt;br /&gt;
This proves that energy is conserved. This can be confirmed experimentally by measuring the kinetic and potential energy in the real experiment, ie measure temperature change and potential energy can be measured using this software.&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;
[[File:ql2817-09.png]]&lt;br /&gt;
&lt;br /&gt;
high translational energy, r(AB)=2, r(BC)=0.74, P AB=-7, P BC=0.5&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-10.png]]&lt;br /&gt;
&lt;br /&gt;
high vibrational energy, r(AB)=2, r(BC)=0.74, P AB=-1, P BC=6&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The reaction is a late TS reaction, also Polanyi&#039;s empirical rules tells us that vibrational energy is more important in compare to vibrational energy in a late transition state reaction, which can also be proved in the graphs above.&lt;br /&gt;
&lt;br /&gt;
==&#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&amp;lt;references/&amp;gt;:&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793673</id>
		<title>MRD:ql2817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:ql2817&amp;diff=793673"/>
		<updated>2019-05-28T10:42:19Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* 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;&lt;br /&gt;
== &#039;&#039;&#039;Question 1&#039;&#039;&#039; ==&lt;br /&gt;
&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;
&lt;br /&gt;
The transition state is defined as the maximum on the minimum energy path linking reactants and the products.It is located at the saddle point in the potential energy surface diagram, which defined as : ∂V(ri)/∂ri=0 and H &amp;lt; 0, where H = frr(r0​,V0​)fVV(r0​,V0​)−f2rV​(r0​,V0​) .&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|The first sentence is correct however your mathematical definition isn&#039;t very clear. Because the TS is a maximum in one direction, the second partial derivative of that function with respect to the TS will be negative, as the second partial derivative of a maximum is always negative. However, it is the maximum on the trajectory of the minimum energy pathway and therefore in the direction that is orthogonal to the reaction trajectory, it is a minimum (in the direction of a cross-section of the well of the pathway) and therefore the second partial derivative will be positive as a second partial derivative of a minimum is always positive. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The transition state is the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|Really not sure what this means, sorry! [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:42, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== 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;
When r(AB)=r(BC)=0.907 Å, p1 = p2 = 0.0, the transition state occurs. The internuclear distance vs time graph gives a relatively straight line which indicates a constant distance.&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the mep and the trajectory you just calculated differ. ===&lt;br /&gt;
The mep trajectory keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy.&lt;br /&gt;
&lt;br /&gt;
r1 = 0.907, r2 = 0.917&lt;br /&gt;
&lt;br /&gt;
Molecules and atome moving away from each other.&lt;br /&gt;
&lt;br /&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;
&lt;br /&gt;
r1 = rts+δ, r2 = rts&lt;br /&gt;
&lt;br /&gt;
final values of the positions r1(t) = 3.45, r2(t) = 0.72 and the average momenta  p1(t) = -1.45, p2(t) = -2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
The molecule and the atom moving close together instead of moving apart.&lt;br /&gt;
&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; border=&amp;quot;5&amp;quot;&lt;br /&gt;
! P1!!P2 !! Etot!! Reactive?!!Description of the dyanmics!!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5|| -99.08|| yes||The trajectory goes through the transition state and also go into the products. ||[[File:Surface01_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5|| -2.0|| -100.22|| no||The trajectory falls back down into the reactants because there was not enough energy for reactants to pass over the transition state. || [[File:Surface02_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5||  -2.5|| -98.91|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface03_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5|| -5.0|| -84.62|| no||The trajectory was carrying enough energy towards products but then it shifts back into the reactants. || [[File:Surface04_ql2817.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5||  -5.2|| -83.40|| yes||The trajectory goes through the transition state and also go into the products with enough energy. || [[File:Surface05_ql2817.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;main&amp;quot;&amp;gt;https://en.wikibooks.org/wiki/Statistical_Thermodynamics_and_Rate_Theories/Eyring_Transition_State_Theory#Assumptions_of_Transition_State_Theory&lt;br /&gt;
&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
*Reactants are in constant equilibrium with the transition state structure.&lt;br /&gt;
*The energy of the particles follow a Boltzmann distribution.&lt;br /&gt;
*Once reactants become the transition state, the transition state structure does not collapse back to the reactants.&lt;br /&gt;
&lt;br /&gt;
Transition state theory will predict a higher reaction rate than experimental one.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;Exercise 2: F-H-H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
===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;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-01.png]]&lt;br /&gt;
&lt;br /&gt;
exothermic, because the trajectory goes from a higher PE to a lower PE.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+F2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB)=1.5,r(BC)=0.74, AB,BC m=0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-02.png]]&lt;br /&gt;
&lt;br /&gt;
endothermic, because the trajectory goes from a lower PE to a higher PE.&lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 1.8108&lt;br /&gt;
r(BC): 0.744877&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-03.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+HF:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB): 0.744877&lt;br /&gt;
r(BC): 1.8108&lt;br /&gt;
AB BC m: 0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-04.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions. ===&lt;br /&gt;
&#039;&#039;&#039;F+H2:&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 30 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-05.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H+FH::&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
activation energy: 0.44kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-06.png]]&lt;br /&gt;
&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;
reactive trajectory:&lt;br /&gt;
&lt;br /&gt;
r(AB):1.6, r(BC):0.74, P AB:-0.5, P BC:0&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-07.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-08.png]]&lt;br /&gt;
&lt;br /&gt;
From the graph above, it is clearly shown that total energy remains the same. Kinetic energy increases to the same extent as potential energy decreases.&lt;br /&gt;
This proves that energy is conserved. This can be confirmed experimentally by measuring the kinetic and potential energy in the real experiment, ie measure temperature change and potential energy can be measured using this software.&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;
[[File:ql2817-09.png]]&lt;br /&gt;
&lt;br /&gt;
high translational energy, r(AB)=2, r(BC)=0.74, P AB=-7, P BC=0.5&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ql2817-10.png]]&lt;br /&gt;
&lt;br /&gt;
high vibrational energy, r(AB)=2, r(BC)=0.74, P AB=-1, P BC=6&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The reaction is a late TS reaction, also Polanyi&#039;s empirical rules tells us that vibrational energy is more important in compare to vibrational energy in a late transition state reaction, which can also be proved in the graphs above.&lt;br /&gt;
&lt;br /&gt;
==&#039;&#039;&#039;References&#039;&#039;&#039;==&lt;br /&gt;
&amp;lt;references/&amp;gt;:&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=JEL3117_MolecularReactionDynamics&amp;diff=793672</id>
		<title>JEL3117 MolecularReactionDynamics</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=JEL3117_MolecularReactionDynamics&amp;diff=793672"/>
		<updated>2019-05-28T10:27:30Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Polanyi&amp;#039;s empirical rule */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Introduction to Molecular Reaction Dynamics ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Energy Curve&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The relative motions of the atoms in a molecule can be described by using an anharmonic oscillator which is derived from a simple harmonic oscillaton. The potential energy curve shows how the potential of the molecule (ex. diatomic molecule) changes as the nuclei are displaced from the equilibrium position which is located at the minimum point of the potential curve. In the diatomic case, the potential energy of the molecule increases exponentially as the separation between the nuclei decreases. As the distance between the nuclei increases, the potential energy of the molecule increases until it reaches the plateau. The difference between the energy of the plateau and the energy of the equilibrium position is the dissociation energy. When the separation is really small, the oscillator follows the simple harmonic oscillator but as the nuclei are further apart, they deviate from the ideality more and follows the anharmonic oscillator.&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_Morse_potential.png|frame|none|Figure 1. A potential energy curve of a diatomic molecule.&amp;lt;ref name=&amp;quot;MorsePotential&amp;quot;/&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
== Exercise 1 : H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
&lt;br /&gt;
In order for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to react with H, the H atom should approach to the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; with a sufficient amount of energy to overcome the activation energy. At the initial condition where time = 0. the bond distance between B and C is represented as r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and the distance between A and B is represented as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; as shown in the diagrams below&lt;br /&gt;
&lt;br /&gt;
[[File:JEL_3117_animation_reactant.png|frame|none|Figure 2. positions of the H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the reactant state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL_3117_animation_product.png|frame|none|Figure 3. positions of the H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the product state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the transition state of a symmetric molecule, 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; should be equal. If there is a sufficient energy to overcome the activation energy, A and B will form a new bond and C will move away as shown above in figure 3.&lt;br /&gt;
&lt;br /&gt;
[[File:JEL_3117_animation_transition_statte.png|frame|none|Figure 4. positions of the H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the transition state.]]&lt;br /&gt;
&lt;br /&gt;
=== Defining transition state in a potential energy surface diagram ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, the transition state is mathematically defined by:&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_state.png]] - (1)&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_state1.png]] - (2)&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_state2.png]] - (3)&lt;br /&gt;
&lt;br /&gt;
All three equations above should be satisfied to identify the transition state. The first condition states that the product of the first derivative of the potential energy with respect to r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and the first derivative of the potential energy with respect to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; should be zero. The second condition states that the second derivative of the potential energy with respect to r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; should be less than zero (meaning maximum point). The third condition states that the second derivative of the potential energy with respect to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; should me more than zero (meaning minimum point). Thus, the transition state is defined as the maximum point on the minimum energy path linking reactants and the products.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This is a really good description. You did not need to include the extra introduction but it is clear that you understand the theory behind the exercise, which is good. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:06, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The transition states are graphically represented below.&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_graph1.png|framed|none|300px|Figure 5. the potential energy curve where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is constant and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is a variable. It shows the minimum energy path along the black line.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_graph2.png|frame|none|Figure 6. the potential energy curve where r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is constant and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is a variable. It shows the maximum energy path.]]&lt;br /&gt;
&lt;br /&gt;
The transition states can be distinguished from a local minimum of the potential energy surface because at the local minimum the second derivative of the potential energy with respect to one of the distances would not give positive value (not a maximum point).&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;
&lt;br /&gt;
The estimated distance transition state position r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is 0.908 Å and this can be shown by &amp;quot;internuclear Distance vs Time&amp;quot; plot as shown below&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_0.98.png|frame|none|Figure 7. internuclear Distance vs Time plot at the transition state position r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
&lt;br /&gt;
At the transition state, I expect the the atoms to vibrate minimum near to zero because the transition state is the stationary maximum point on the minimum energy path. As the they vibrate more and more, they will slide down the potential surface curve and separate to form either product or reactant.&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;
&lt;br /&gt;
[[File:JEL3117_transition1_MEP.png|frame|none|Figure 8. contour plot of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 in MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_MEP_momentavstime_graph.png|frame|none|Figure 9. momentum vs time graph of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 in MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition1_DYNAMIC.png|frame|none|Figure 10. contour plot of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 in Dynamic.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_DYNAMIC_momentavstime_graph.png|frame|none|Figure 11. surface plot of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 in Dynamic.]]&lt;br /&gt;
&lt;br /&gt;
The above graphs were plotted by setting r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0 kg m/s.&lt;br /&gt;
 &lt;br /&gt;
the first two graphs show the reaction path of the reaction with the MEP mode. MEP sets the momenta and velocities of the molecule to zero (shown in figure 9) in each time every step and process the reaction in a infinitely slow motion. The last two graphs show the reaction path of the reaction with the dynamics mode. Dynamics shows the vibrational motion of the molecule which is derived from the internal energy of the molecule. Thus, oscillation of the energy of the reaction path is shown in the potential energy surface. By setting the momentum to zero at every point, the reaction path will stop when the exchange of the atoms is completed. However, when the momentum is not zero, the products will move away from each other continuously due to conservation of momentum. This is shown in figure 8 and 10 where the reaction path ends earlier for MEP than Dynamics. &lt;br /&gt;
&lt;br /&gt;
If r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.908 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.909 Å, A and B would form the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and C would move away from the molecule. Thus, the reaction path would head towards the other end of the contour plot.&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_DYNAMIC_intermolecular.png|frame|none|Figure 12. Intermolecular distance vs time graph of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.908, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.909.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_DYNAMIC_Momenta.png|frame|none|Figure 13. momenta vs time graph of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.908, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.909.]]&lt;br /&gt;
&lt;br /&gt;
Figure 12 shows that the distance between B and C increases but the distance between A and B decreases with a little oscillation. Moreover, Figure 13 shows that the momentum of BC increases then reaches the plateau which means that the B and C are separated and the momentum of AB increases then start to oscillate as it plateaus. It means that AB bonds are formed and they are oscillating. Thus, the above data supports that AB bond is formed instead of BC bond when 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; are reversed&lt;br /&gt;
&lt;br /&gt;
=== Reactive and unreactive trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Reactive and unreactive trajectories&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&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;
| -1.25 || -2.5 || -99.018 || Reactive || Initially, C approaches AB molecule. As C approaches, the distance between A and B remains almost constant with no oscillations and the potential energy between B and C increases. As it reaches the transition state, the system has an enough kinetic energy to overcome the activation energy. Therefore, a new BC bond is formed and the AB bond is broken. Then, as the reaction path passes the transition state, the BC molecule oscillates and A moves away from the new product BC.   || [[File:JEL3117_reactive_nonreactive_contour_first.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || Initially, the AB molecule oscillates and C approaches AB molecule. As the reaction path reaches the transition state, the system does not have an enough amount of energy to overcome the activation energy and the new BC bond is not formed. Thus, C moves away from the AB molecule and AB molecule remains oscillating and keep their bonds. ||[[File:JEL3117_reactive_nonreactive_contour_second.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || Initially, the AB molecule oscillates and C approaches the AB molecule. As the reaction path reaches the transition state, the system has the enough energy to overcome the activation energy and a new BC bond is formed and A moves away from the product as the reaction proceeds.  || [[File:JEL3117_reactive_nonreactive_contour_third.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Unreactive || Initially, the AB molecule does not oscillate and C approaches the molecule AB. As the reaction approaches the transition state, the system has an enough energy to overcome the transition state and the new BC bond is formed and A moves away from the BC molecule. However, the oscillation of the BC bond is too big such that the BC bond is broken and AB bond is formed again. As a result, the AB molecule remains as it is and C moves away from the AB molecule. || [[File:JEL3117_reactive_nonreactive_contour_fourth.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || Initially, the AB molecules does not oscillate and C approaches the molecule. As the reaction approaches the transition state, the AB molecule starts to oscillate dramatically such that AB bond is broken. As a result,the BC bond is formed and A moves away from the the molecule BC || [[File:JEL3117_reactive_nonreactive_contour_fifth.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the table, it can be concluded that activation energy is not the only factor that affects the success of the reaction but other factors such as collision in a correct geometry also contributes to the success of the reaction.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|OK, this is the right idea - total energy isn&#039;t enough to dictate whether or not a system will be reactive. However, where have you got this idea of geometry from? It&#039;s true that geometry can affect reaction success but your table doesn&#039;t show this. You either need to explain what you mean if this is from your own scientific instinct or you need to cite a literature reference. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:13, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition state Theory ===&lt;br /&gt;
&lt;br /&gt;
The main assumptions of transition state theory are as follows&amp;lt;ref name=&amp;quot;transition state&amp;quot;/&amp;gt; :&lt;br /&gt;
&lt;br /&gt;
1, For each elementary step in a multi-step reaction, the intermediates are long lived enough to reach a Boltzmann distribution of energies before proceeding to the next step.&lt;br /&gt;
&lt;br /&gt;
2, The atomic nuclei behave according to the classic mechanics.&lt;br /&gt;
&lt;br /&gt;
3, The reaction is successful if the reaction path passes over the lowest energy saddle point on the potential energy surface (transition state).&lt;br /&gt;
&lt;br /&gt;
However, in reality, the assumptions start to break down. The transition states are very short lived and the Boltzmann distribution of energies at each step near activated complexes is hard to be obtained. Moreover, in reality, atoms behave in a quantum mechanical manner and the reaction might be successful to form the product even though the energy of the reactants is not enough to overcome the activation energy via quantum tunnelling. Moreover, in reality, the transition state is not necessarily at the lowest saddle point at high temperatures. Thus, there are alternative pathway to the reaction.&lt;br /&gt;
&lt;br /&gt;
As a result, the predicted reaction rate values by using Transition State Theory would be lower than the experimental values due to limitations of the assumptions.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| You are very close to the right idea in point 3 but you haven&#039;t quite followed the thought through to completion. This assumption (point 3) means that TST does not account for the idea of barrier recrossing. I.e. in TST once a molecule has hit the TS, that&#039;s it, the reaction is successful. In reality, the molecule can go back to the reactants side, and then over the TS to the product side, and dance around over the TS for a bit. This means that TST predicts that the rate from TST would be higher than in real life (reaction occurs quicker) as it doesn&#039;t account for this extra time spent at the TS. So TST overpredicts the rate constant. &lt;br /&gt;
&lt;br /&gt;
Also note that tunelling is not accounted for in this experiment, and also tunneling would accelerate the reaction relative to theoretical prediction (no tunneling) and therefore would have the opposite effect to the barrier recrossing scenario. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:22, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 : F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
=== PES inspection ===&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_F_HH_potential_curve1.png|frame|none|Figure 14. the potential energy surface of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_H_HF_potential_curve1.png|frame|none|Figure 15. the potential energy surface of H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
Based on the potential energy surfaces, the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic because the energy of the reactant is higher than the energy of the product and the H + HF reaction is endothermic because the energy of the product is higher than the energy of the reactant.&lt;br /&gt;
&lt;br /&gt;
This means that the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is weaker than the bond strength of HF because the energy released from breaking H-H bond is lower than the energy required to form the H-F bond for the endothermic F + HF reaction and the energy released from breaking H-F bond is higher than the energy required to form the H-H bond for the exothermic F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction .&lt;br /&gt;
&lt;br /&gt;
=== Approximate Position of the transition state ===&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_F_H2_approximate_TS_intermoleculardistance2.png|frame|none|Figure 16. The intermolecular distance vs time graph of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_F_H2_approximate_TS_potential_surface2.png|frame|none|Figure 17. The potential energy surface of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction indicating the approximate position of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Based on the Hammond&#039;s postulate, the transition state of the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; lies near the reactant. Looking at  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; graph, the transition state therefore lies near the reactant and it is supported by the intermolecular vs time graph as shown above (No change in the intermolecular distances for a subsequent period of time). Likewise, the transition state of the endothermic H + HF reaction lies near the product.&lt;br /&gt;
&lt;br /&gt;
With trial and errors, the position of the transition state for the exothermic F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction was found at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;(AB Distance) = 1.8106929 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(BC Distance) = 0.745 Å.&lt;br /&gt;
&lt;br /&gt;
The position of the transition state for the endothermic H + HF reaction was found at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;(AB Distance) = 0.745 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(BC Distance) = 1.8106929 Å.&lt;br /&gt;
&lt;br /&gt;
The activation energies of both of the reactions were found by displacing the activated complex slightly from the transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:JEL_3117_energy_time_graph_exothermic.png|frame|none|Figure 18. Energy vs time graph of the exothermic reaction which illustrates the activation energy of the reaction.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL_3117_energy_time_graph_endothermic.png|frame|none|Figure 19. Energy vs time graph of the endothermic reaction which illustrates the activation energy of the reaction.]]&lt;br /&gt;
&lt;br /&gt;
The activation energy of the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; was calculated by displacing r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; to 1.8107 Å. However, the activation energy of the exothermic reaction was negligible such that was hard to be observed from the energy vs time graph.&lt;br /&gt;
&lt;br /&gt;
The activation energy of the endothermic reaction was calculated by displacing r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to 1.8106 Å. The activation energy was found as 29.5 KJ/mol. &lt;br /&gt;
&lt;br /&gt;
=== Reaction Dynamics ===&lt;br /&gt;
&lt;br /&gt;
By the conservation of energy, the total energy is always conserved. At the start, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and  and F atom are stationary thus they only have potential energies. As they are brought together, the potential energies between them decrease and the kinetic energies of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F atom subsequently increase. As they collide, they start to oscillate and H-H bond is broken and new H-F bond is formed. Since the reaction is exothermic, the excess energy is released from the reaction as heat and the remaining energy is converted to the vibrational energy of HF molecule and kinetic energy of H atom.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|How can the potential energy of the system be decreasing as it goes up the hill of the TS? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:25, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Experimentally, the above mechanism can be confirmed by measuring the heat released during the reaction with a calorimeter and the vibrational energy of HF molecule can be measured by using IR. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This answer is not quite complete. What is calorimetry? What does it measure, and why can it be applied here? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:25, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
[[File:JEL_3117_momentum_time_graph_exothermic.png|frame|none|Figure 19. Energy vs time graph of the endothermic reaction which illustrates the activation energy of the reaction.]]&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s empirical rule ===&lt;br /&gt;
&lt;br /&gt;
The position of the transition state is important in determining the distribution of energy between different modes. For the early transition (exothermic reaction), having translational energy in majority is sufficient to form the product because having vibrational energy would cause the molecule to slide the potential energy surface side to side such that it does not have enough energy to overcome the activation energy. However, for the late transition (endothermic reaction, having vibrational energy helps to climb the potential energy surface up to the transition state. Having too much vibrational energy bounces back the product to the reactant.&amp;lt;ref name=&amp;quot;polany&#039;s rule&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| All good, but how does this manifest in your observations during these exercises? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:27, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| Overall these answers are very detailed and thorough - any question where I have not made a comment you can assume your answer is very good! [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:27, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;MorsePotential&amp;quot;&amp;gt; Chemistry LibreTexts. &#039;&#039;The Morse Potential graph&#039;&#039;. Available from : https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Map%3A_Physical_Chemistry_(McQuarrie_and_Simon)/05._The_Harmonic_Oscillator_and_the_Rigid_Rotator%3A_Two_Spectroscopic_Models/5.3%3A_The_Harmonic_Oscillator_Approximates_Vibrations &amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;transition state&amp;quot;&amp;gt; &lt;br /&gt;
Atkins, P.W., and Paula J. De. &#039;&#039;Atkin&#039;s Physical Chemistry&#039;&#039;. Oxford: Oxford University Press. 2006&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;polany&#039;s rule&amp;quot;&amp;gt; Jeffrey I.Steinfeld, Joseph S. Francisco, William L.Hase. &#039;&#039;Chemical Kinetics and Dynamics&#039;&#039;. United States: A Paramount Communications Company, 1989 &amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=JEL3117_MolecularReactionDynamics&amp;diff=793671</id>
		<title>JEL3117 MolecularReactionDynamics</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=JEL3117_MolecularReactionDynamics&amp;diff=793671"/>
		<updated>2019-05-28T10:25:51Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Introduction to Molecular Reaction Dynamics ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Energy Curve&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The relative motions of the atoms in a molecule can be described by using an anharmonic oscillator which is derived from a simple harmonic oscillaton. The potential energy curve shows how the potential of the molecule (ex. diatomic molecule) changes as the nuclei are displaced from the equilibrium position which is located at the minimum point of the potential curve. In the diatomic case, the potential energy of the molecule increases exponentially as the separation between the nuclei decreases. As the distance between the nuclei increases, the potential energy of the molecule increases until it reaches the plateau. The difference between the energy of the plateau and the energy of the equilibrium position is the dissociation energy. When the separation is really small, the oscillator follows the simple harmonic oscillator but as the nuclei are further apart, they deviate from the ideality more and follows the anharmonic oscillator.&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_Morse_potential.png|frame|none|Figure 1. A potential energy curve of a diatomic molecule.&amp;lt;ref name=&amp;quot;MorsePotential&amp;quot;/&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
== Exercise 1 : H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
&lt;br /&gt;
In order for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to react with H, the H atom should approach to the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; with a sufficient amount of energy to overcome the activation energy. At the initial condition where time = 0. the bond distance between B and C is represented as r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and the distance between A and B is represented as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; as shown in the diagrams below&lt;br /&gt;
&lt;br /&gt;
[[File:JEL_3117_animation_reactant.png|frame|none|Figure 2. positions of the H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the reactant state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL_3117_animation_product.png|frame|none|Figure 3. positions of the H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the product state.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the transition state of a symmetric molecule, 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; should be equal. If there is a sufficient energy to overcome the activation energy, A and B will form a new bond and C will move away as shown above in figure 3.&lt;br /&gt;
&lt;br /&gt;
[[File:JEL_3117_animation_transition_statte.png|frame|none|Figure 4. positions of the H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the transition state.]]&lt;br /&gt;
&lt;br /&gt;
=== Defining transition state in a potential energy surface diagram ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, the transition state is mathematically defined by:&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_state.png]] - (1)&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_state1.png]] - (2)&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_state2.png]] - (3)&lt;br /&gt;
&lt;br /&gt;
All three equations above should be satisfied to identify the transition state. The first condition states that the product of the first derivative of the potential energy with respect to r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and the first derivative of the potential energy with respect to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; should be zero. The second condition states that the second derivative of the potential energy with respect to r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; should be less than zero (meaning maximum point). The third condition states that the second derivative of the potential energy with respect to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; should me more than zero (meaning minimum point). Thus, the transition state is defined as the maximum point on the minimum energy path linking reactants and the products.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This is a really good description. You did not need to include the extra introduction but it is clear that you understand the theory behind the exercise, which is good. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:06, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
The transition states are graphically represented below.&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_graph1.png|framed|none|300px|Figure 5. the potential energy curve where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is constant and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is a variable. It shows the minimum energy path along the black line.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_graph2.png|frame|none|Figure 6. the potential energy curve where r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is constant and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is a variable. It shows the maximum energy path.]]&lt;br /&gt;
&lt;br /&gt;
The transition states can be distinguished from a local minimum of the potential energy surface because at the local minimum the second derivative of the potential energy with respect to one of the distances would not give positive value (not a maximum point).&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;
&lt;br /&gt;
The estimated distance transition state position r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is 0.908 Å and this can be shown by &amp;quot;internuclear Distance vs Time&amp;quot; plot as shown below&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_0.98.png|frame|none|Figure 7. internuclear Distance vs Time plot at the transition state position r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
&lt;br /&gt;
At the transition state, I expect the the atoms to vibrate minimum near to zero because the transition state is the stationary maximum point on the minimum energy path. As the they vibrate more and more, they will slide down the potential surface curve and separate to form either product or reactant.&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;
&lt;br /&gt;
[[File:JEL3117_transition1_MEP.png|frame|none|Figure 8. contour plot of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 in MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_MEP_momentavstime_graph.png|frame|none|Figure 9. momentum vs time graph of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 in MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition1_DYNAMIC.png|frame|none|Figure 10. contour plot of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 in Dynamic.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_DYNAMIC_momentavstime_graph.png|frame|none|Figure 11. surface plot of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 in Dynamic.]]&lt;br /&gt;
&lt;br /&gt;
The above graphs were plotted by setting r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0 kg m/s.&lt;br /&gt;
 &lt;br /&gt;
the first two graphs show the reaction path of the reaction with the MEP mode. MEP sets the momenta and velocities of the molecule to zero (shown in figure 9) in each time every step and process the reaction in a infinitely slow motion. The last two graphs show the reaction path of the reaction with the dynamics mode. Dynamics shows the vibrational motion of the molecule which is derived from the internal energy of the molecule. Thus, oscillation of the energy of the reaction path is shown in the potential energy surface. By setting the momentum to zero at every point, the reaction path will stop when the exchange of the atoms is completed. However, when the momentum is not zero, the products will move away from each other continuously due to conservation of momentum. This is shown in figure 8 and 10 where the reaction path ends earlier for MEP than Dynamics. &lt;br /&gt;
&lt;br /&gt;
If r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.908 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.909 Å, A and B would form the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and C would move away from the molecule. Thus, the reaction path would head towards the other end of the contour plot.&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_DYNAMIC_intermolecular.png|frame|none|Figure 12. Intermolecular distance vs time graph of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.908, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.909.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_transition_DYNAMIC_Momenta.png|frame|none|Figure 13. momenta vs time graph of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.908, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.909.]]&lt;br /&gt;
&lt;br /&gt;
Figure 12 shows that the distance between B and C increases but the distance between A and B decreases with a little oscillation. Moreover, Figure 13 shows that the momentum of BC increases then reaches the plateau which means that the B and C are separated and the momentum of AB increases then start to oscillate as it plateaus. It means that AB bonds are formed and they are oscillating. Thus, the above data supports that AB bond is formed instead of BC bond when 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; are reversed&lt;br /&gt;
&lt;br /&gt;
=== Reactive and unreactive trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Reactive and unreactive trajectories&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&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;
| -1.25 || -2.5 || -99.018 || Reactive || Initially, C approaches AB molecule. As C approaches, the distance between A and B remains almost constant with no oscillations and the potential energy between B and C increases. As it reaches the transition state, the system has an enough kinetic energy to overcome the activation energy. Therefore, a new BC bond is formed and the AB bond is broken. Then, as the reaction path passes the transition state, the BC molecule oscillates and A moves away from the new product BC.   || [[File:JEL3117_reactive_nonreactive_contour_first.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || Initially, the AB molecule oscillates and C approaches AB molecule. As the reaction path reaches the transition state, the system does not have an enough amount of energy to overcome the activation energy and the new BC bond is not formed. Thus, C moves away from the AB molecule and AB molecule remains oscillating and keep their bonds. ||[[File:JEL3117_reactive_nonreactive_contour_second.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || Initially, the AB molecule oscillates and C approaches the AB molecule. As the reaction path reaches the transition state, the system has the enough energy to overcome the activation energy and a new BC bond is formed and A moves away from the product as the reaction proceeds.  || [[File:JEL3117_reactive_nonreactive_contour_third.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Unreactive || Initially, the AB molecule does not oscillate and C approaches the molecule AB. As the reaction approaches the transition state, the system has an enough energy to overcome the transition state and the new BC bond is formed and A moves away from the BC molecule. However, the oscillation of the BC bond is too big such that the BC bond is broken and AB bond is formed again. As a result, the AB molecule remains as it is and C moves away from the AB molecule. || [[File:JEL3117_reactive_nonreactive_contour_fourth.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || Initially, the AB molecules does not oscillate and C approaches the molecule. As the reaction approaches the transition state, the AB molecule starts to oscillate dramatically such that AB bond is broken. As a result,the BC bond is formed and A moves away from the the molecule BC || [[File:JEL3117_reactive_nonreactive_contour_fifth.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the table, it can be concluded that activation energy is not the only factor that affects the success of the reaction but other factors such as collision in a correct geometry also contributes to the success of the reaction.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|OK, this is the right idea - total energy isn&#039;t enough to dictate whether or not a system will be reactive. However, where have you got this idea of geometry from? It&#039;s true that geometry can affect reaction success but your table doesn&#039;t show this. You either need to explain what you mean if this is from your own scientific instinct or you need to cite a literature reference. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:13, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
=== Transition state Theory ===&lt;br /&gt;
&lt;br /&gt;
The main assumptions of transition state theory are as follows&amp;lt;ref name=&amp;quot;transition state&amp;quot;/&amp;gt; :&lt;br /&gt;
&lt;br /&gt;
1, For each elementary step in a multi-step reaction, the intermediates are long lived enough to reach a Boltzmann distribution of energies before proceeding to the next step.&lt;br /&gt;
&lt;br /&gt;
2, The atomic nuclei behave according to the classic mechanics.&lt;br /&gt;
&lt;br /&gt;
3, The reaction is successful if the reaction path passes over the lowest energy saddle point on the potential energy surface (transition state).&lt;br /&gt;
&lt;br /&gt;
However, in reality, the assumptions start to break down. The transition states are very short lived and the Boltzmann distribution of energies at each step near activated complexes is hard to be obtained. Moreover, in reality, atoms behave in a quantum mechanical manner and the reaction might be successful to form the product even though the energy of the reactants is not enough to overcome the activation energy via quantum tunnelling. Moreover, in reality, the transition state is not necessarily at the lowest saddle point at high temperatures. Thus, there are alternative pathway to the reaction.&lt;br /&gt;
&lt;br /&gt;
As a result, the predicted reaction rate values by using Transition State Theory would be lower than the experimental values due to limitations of the assumptions.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink| You are very close to the right idea in point 3 but you haven&#039;t quite followed the thought through to completion. This assumption (point 3) means that TST does not account for the idea of barrier recrossing. I.e. in TST once a molecule has hit the TS, that&#039;s it, the reaction is successful. In reality, the molecule can go back to the reactants side, and then over the TS to the product side, and dance around over the TS for a bit. This means that TST predicts that the rate from TST would be higher than in real life (reaction occurs quicker) as it doesn&#039;t account for this extra time spent at the TS. So TST overpredicts the rate constant. &lt;br /&gt;
&lt;br /&gt;
Also note that tunelling is not accounted for in this experiment, and also tunneling would accelerate the reaction relative to theoretical prediction (no tunneling) and therefore would have the opposite effect to the barrier recrossing scenario. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:22, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 : F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
=== PES inspection ===&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_F_HH_potential_curve1.png|frame|none|Figure 14. the potential energy surface of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_H_HF_potential_curve1.png|frame|none|Figure 15. the potential energy surface of H + HF reaction]]&lt;br /&gt;
&lt;br /&gt;
Based on the potential energy surfaces, the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic because the energy of the reactant is higher than the energy of the product and the H + HF reaction is endothermic because the energy of the product is higher than the energy of the reactant.&lt;br /&gt;
&lt;br /&gt;
This means that the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is weaker than the bond strength of HF because the energy released from breaking H-H bond is lower than the energy required to form the H-F bond for the endothermic F + HF reaction and the energy released from breaking H-F bond is higher than the energy required to form the H-H bond for the exothermic F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction .&lt;br /&gt;
&lt;br /&gt;
=== Approximate Position of the transition state ===&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_F_H2_approximate_TS_intermoleculardistance2.png|frame|none|Figure 16. The intermolecular distance vs time graph of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL3117_F_H2_approximate_TS_potential_surface2.png|frame|none|Figure 17. The potential energy surface of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction indicating the approximate position of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Based on the Hammond&#039;s postulate, the transition state of the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; lies near the reactant. Looking at  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; graph, the transition state therefore lies near the reactant and it is supported by the intermolecular vs time graph as shown above (No change in the intermolecular distances for a subsequent period of time). Likewise, the transition state of the endothermic H + HF reaction lies near the product.&lt;br /&gt;
&lt;br /&gt;
With trial and errors, the position of the transition state for the exothermic F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction was found at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;(AB Distance) = 1.8106929 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(BC Distance) = 0.745 Å.&lt;br /&gt;
&lt;br /&gt;
The position of the transition state for the endothermic H + HF reaction was found at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;(AB Distance) = 0.745 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(BC Distance) = 1.8106929 Å.&lt;br /&gt;
&lt;br /&gt;
The activation energies of both of the reactions were found by displacing the activated complex slightly from the transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:JEL_3117_energy_time_graph_exothermic.png|frame|none|Figure 18. Energy vs time graph of the exothermic reaction which illustrates the activation energy of the reaction.]]&lt;br /&gt;
&lt;br /&gt;
[[File:JEL_3117_energy_time_graph_endothermic.png|frame|none|Figure 19. Energy vs time graph of the endothermic reaction which illustrates the activation energy of the reaction.]]&lt;br /&gt;
&lt;br /&gt;
The activation energy of the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; was calculated by displacing r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; to 1.8107 Å. However, the activation energy of the exothermic reaction was negligible such that was hard to be observed from the energy vs time graph.&lt;br /&gt;
&lt;br /&gt;
The activation energy of the endothermic reaction was calculated by displacing r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to 1.8106 Å. The activation energy was found as 29.5 KJ/mol. &lt;br /&gt;
&lt;br /&gt;
=== Reaction Dynamics ===&lt;br /&gt;
&lt;br /&gt;
By the conservation of energy, the total energy is always conserved. At the start, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and  and F atom are stationary thus they only have potential energies. As they are brought together, the potential energies between them decrease and the kinetic energies of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F atom subsequently increase. As they collide, they start to oscillate and H-H bond is broken and new H-F bond is formed. Since the reaction is exothermic, the excess energy is released from the reaction as heat and the remaining energy is converted to the vibrational energy of HF molecule and kinetic energy of H atom.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|How can the potential energy of the system be decreasing as it goes up the hill of the TS? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:25, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
Experimentally, the above mechanism can be confirmed by measuring the heat released during the reaction with a calorimeter and the vibrational energy of HF molecule can be measured by using IR. &lt;br /&gt;
&lt;br /&gt;
{{fontcolor|pink|This answer is not quite complete. What is calorimetry? What does it measure, and why can it be applied here? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:25, 28 May 2019 (BST)}}&lt;br /&gt;
&lt;br /&gt;
[[File:JEL_3117_momentum_time_graph_exothermic.png|frame|none|Figure 19. Energy vs time graph of the endothermic reaction which illustrates the activation energy of the reaction.]]&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s empirical rule ===&lt;br /&gt;
&lt;br /&gt;
The position of the transition state is important in determining the distribution of energy between different modes. For the early transition (exothermic reaction), having translational energy in majority is sufficient to form the product because having vibrational energy would cause the molecule to slide the potential energy surface side to side such that it does not have enough energy to overcome the activation energy. However, for the late transition (endothermic reaction, having vibrational energy helps to climb the potential energy surface up to the transition state. Having too much vibrational energy bounces back the product to the reactant.&amp;lt;ref name=&amp;quot;polany&#039;s rule&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;MorsePotential&amp;quot;&amp;gt; Chemistry LibreTexts. &#039;&#039;The Morse Potential graph&#039;&#039;. Available from : https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Map%3A_Physical_Chemistry_(McQuarrie_and_Simon)/05._The_Harmonic_Oscillator_and_the_Rigid_Rotator%3A_Two_Spectroscopic_Models/5.3%3A_The_Harmonic_Oscillator_Approximates_Vibrations &amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;transition state&amp;quot;&amp;gt; &lt;br /&gt;
Atkins, P.W., and Paula J. De. &#039;&#039;Atkin&#039;s Physical Chemistry&#039;&#039;. Oxford: Oxford University Press. 2006&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;polany&#039;s rule&amp;quot;&amp;gt; Jeffrey I.Steinfeld, Joseph S. Francisco, William L.Hase. &#039;&#039;Chemical Kinetics and Dynamics&#039;&#039;. United States: A Paramount Communications Company, 1989 &amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=JEL3117_MolecularReactionDynamics&amp;diff=793670</id>
		<title>JEL3117 MolecularReactionDynamics</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=JEL3117_MolecularReactionDynamics&amp;diff=793670"/>
		<updated>2019-05-28T10:25:15Z</updated>

		<summary type="html">&lt;p&gt;Rk2918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Introduction to Molecular Reaction Dynamics ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Potential Energy Curve&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The relative motions of the atoms in a molecule can be described by using an anharmonic oscillator which is derived from a simple harmonic oscillaton. The potential energy curve shows how the potential of the molecule (ex. diatomic molecule) changes as the nuclei are displaced from the equilibrium position which is located at the minimum point of the potential curve. In the diatomic case, the potential energy of the molecule increases exponentially as the separation between the nuclei decreases. As the distance between the nuclei increases, the potential energy of the molecule increases until it reaches the plateau. The difference between the energy of the plateau and the energy of the equilibrium position is the dissociation energy. When the separation is really small, the oscillator follows the simple harmonic oscillator but as the nuclei are further apart, they deviate from the ideality more and follows the anharmonic oscillator.&lt;br /&gt;
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[[File:JEL3117_Morse_potential.png|frame|none|Figure 1. A potential energy curve of a diatomic molecule.&amp;lt;ref name=&amp;quot;MorsePotential&amp;quot;/&amp;gt;]]&lt;br /&gt;
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== Exercise 1 : H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
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In order for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to react with H, the H atom should approach to the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; with a sufficient amount of energy to overcome the activation energy. At the initial condition where time = 0. the bond distance between B and C is represented as r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and the distance between A and B is represented as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; as shown in the diagrams below&lt;br /&gt;
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[[File:JEL_3117_animation_reactant.png|frame|none|Figure 2. positions of the H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the reactant state.]]&lt;br /&gt;
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[[File:JEL_3117_animation_product.png|frame|none|Figure 3. positions of the H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the product state.]]&lt;br /&gt;
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For the transition state of a symmetric molecule, 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; should be equal. If there is a sufficient energy to overcome the activation energy, A and B will form a new bond and C will move away as shown above in figure 3.&lt;br /&gt;
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[[File:JEL_3117_animation_transition_statte.png|frame|none|Figure 4. positions of the H and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the transition state.]]&lt;br /&gt;
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=== Defining transition state in a potential energy surface diagram ===&lt;br /&gt;
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On a potential energy surface diagram, the transition state is mathematically defined by:&lt;br /&gt;
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[[File:JEL3117_transition_state.png]] - (1)&lt;br /&gt;
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[[File:JEL3117_transition_state1.png]] - (2)&lt;br /&gt;
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[[File:JEL3117_transition_state2.png]] - (3)&lt;br /&gt;
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All three equations above should be satisfied to identify the transition state. The first condition states that the product of the first derivative of the potential energy with respect to r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and the first derivative of the potential energy with respect to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; should be zero. The second condition states that the second derivative of the potential energy with respect to r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; should be less than zero (meaning maximum point). The third condition states that the second derivative of the potential energy with respect to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; should me more than zero (meaning minimum point). Thus, the transition state is defined as the maximum point on the minimum energy path linking reactants and the products.&lt;br /&gt;
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{{fontcolor|pink|This is a really good description. You did not need to include the extra introduction but it is clear that you understand the theory behind the exercise, which is good. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:06, 28 May 2019 (BST)}}&lt;br /&gt;
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The transition states are graphically represented below.&lt;br /&gt;
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[[File:JEL3117_transition_graph1.png|framed|none|300px|Figure 5. the potential energy curve where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is constant and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is a variable. It shows the minimum energy path along the black line.]]&lt;br /&gt;
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[[File:JEL3117_transition_graph2.png|frame|none|Figure 6. the potential energy curve where r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is constant and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is a variable. It shows the maximum energy path.]]&lt;br /&gt;
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The transition states can be distinguished from a local minimum of the potential energy surface because at the local minimum the second derivative of the potential energy with respect to one of the distances would not give positive value (not a maximum point).&lt;br /&gt;
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=== 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;
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The estimated distance transition state position r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is 0.908 Å and this can be shown by &amp;quot;internuclear Distance vs Time&amp;quot; plot as shown below&lt;br /&gt;
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[[File:JEL3117_transition_0.98.png|frame|none|Figure 7. internuclear Distance vs Time plot at the transition state position r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
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At the transition state, I expect the the atoms to vibrate minimum near to zero because the transition state is the stationary maximum point on the minimum energy path. As the they vibrate more and more, they will slide down the potential surface curve and separate to form either product or reactant.&lt;br /&gt;
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=== 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;
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[[File:JEL3117_transition1_MEP.png|frame|none|Figure 8. contour plot of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 in MEP.]]&lt;br /&gt;
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[[File:JEL3117_transition_MEP_momentavstime_graph.png|frame|none|Figure 9. momentum vs time graph of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 in MEP.]]&lt;br /&gt;
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[[File:JEL3117_transition1_DYNAMIC.png|frame|none|Figure 10. contour plot of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 in Dynamic.]]&lt;br /&gt;
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[[File:JEL3117_transition_DYNAMIC_momentavstime_graph.png|frame|none|Figure 11. surface plot of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 in Dynamic.]]&lt;br /&gt;
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The above graphs were plotted by setting r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.909 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.908 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0 kg m/s.&lt;br /&gt;
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the first two graphs show the reaction path of the reaction with the MEP mode. MEP sets the momenta and velocities of the molecule to zero (shown in figure 9) in each time every step and process the reaction in a infinitely slow motion. The last two graphs show the reaction path of the reaction with the dynamics mode. Dynamics shows the vibrational motion of the molecule which is derived from the internal energy of the molecule. Thus, oscillation of the energy of the reaction path is shown in the potential energy surface. By setting the momentum to zero at every point, the reaction path will stop when the exchange of the atoms is completed. However, when the momentum is not zero, the products will move away from each other continuously due to conservation of momentum. This is shown in figure 8 and 10 where the reaction path ends earlier for MEP than Dynamics. &lt;br /&gt;
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If r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.908 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.909 Å, A and B would form the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and C would move away from the molecule. Thus, the reaction path would head towards the other end of the contour plot.&lt;br /&gt;
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[[File:JEL3117_transition_DYNAMIC_intermolecular.png|frame|none|Figure 12. Intermolecular distance vs time graph of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.908, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.909.]]&lt;br /&gt;
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[[File:JEL3117_transition_DYNAMIC_Momenta.png|frame|none|Figure 13. momenta vs time graph of the reaction H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = 0.908, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.909.]]&lt;br /&gt;
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Figure 12 shows that the distance between B and C increases but the distance between A and B decreases with a little oscillation. Moreover, Figure 13 shows that the momentum of BC increases then reaches the plateau which means that the B and C are separated and the momentum of AB increases then start to oscillate as it plateaus. It means that AB bonds are formed and they are oscillating. Thus, the above data supports that AB bond is formed instead of BC bond when 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; are reversed&lt;br /&gt;
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=== Reactive and unreactive trajectories ===&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Reactive and unreactive trajectories&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&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;
| -1.25 || -2.5 || -99.018 || Reactive || Initially, C approaches AB molecule. As C approaches, the distance between A and B remains almost constant with no oscillations and the potential energy between B and C increases. As it reaches the transition state, the system has an enough kinetic energy to overcome the activation energy. Therefore, a new BC bond is formed and the AB bond is broken. Then, as the reaction path passes the transition state, the BC molecule oscillates and A moves away from the new product BC.   || [[File:JEL3117_reactive_nonreactive_contour_first.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || Initially, the AB molecule oscillates and C approaches AB molecule. As the reaction path reaches the transition state, the system does not have an enough amount of energy to overcome the activation energy and the new BC bond is not formed. Thus, C moves away from the AB molecule and AB molecule remains oscillating and keep their bonds. ||[[File:JEL3117_reactive_nonreactive_contour_second.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || Initially, the AB molecule oscillates and C approaches the AB molecule. As the reaction path reaches the transition state, the system has the enough energy to overcome the activation energy and a new BC bond is formed and A moves away from the product as the reaction proceeds.  || [[File:JEL3117_reactive_nonreactive_contour_third.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Unreactive || Initially, the AB molecule does not oscillate and C approaches the molecule AB. As the reaction approaches the transition state, the system has an enough energy to overcome the transition state and the new BC bond is formed and A moves away from the BC molecule. However, the oscillation of the BC bond is too big such that the BC bond is broken and AB bond is formed again. As a result, the AB molecule remains as it is and C moves away from the AB molecule. || [[File:JEL3117_reactive_nonreactive_contour_fourth.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || Initially, the AB molecules does not oscillate and C approaches the molecule. As the reaction approaches the transition state, the AB molecule starts to oscillate dramatically such that AB bond is broken. As a result,the BC bond is formed and A moves away from the the molecule BC || [[File:JEL3117_reactive_nonreactive_contour_fifth.png]]&lt;br /&gt;
|}&lt;br /&gt;
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From the table, it can be concluded that activation energy is not the only factor that affects the success of the reaction but other factors such as collision in a correct geometry also contributes to the success of the reaction.&lt;br /&gt;
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{{fontcolor|pink|OK, this is the right idea - total energy isn&#039;t enough to dictate whether or not a system will be reactive. However, where have you got this idea of geometry from? It&#039;s true that geometry can affect reaction success but your table doesn&#039;t show this. You either need to explain what you mean if this is from your own scientific instinct or you need to cite a literature reference. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:13, 28 May 2019 (BST)}}&lt;br /&gt;
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=== Transition state Theory ===&lt;br /&gt;
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The main assumptions of transition state theory are as follows&amp;lt;ref name=&amp;quot;transition state&amp;quot;/&amp;gt; :&lt;br /&gt;
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1, For each elementary step in a multi-step reaction, the intermediates are long lived enough to reach a Boltzmann distribution of energies before proceeding to the next step.&lt;br /&gt;
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2, The atomic nuclei behave according to the classic mechanics.&lt;br /&gt;
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3, The reaction is successful if the reaction path passes over the lowest energy saddle point on the potential energy surface (transition state).&lt;br /&gt;
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However, in reality, the assumptions start to break down. The transition states are very short lived and the Boltzmann distribution of energies at each step near activated complexes is hard to be obtained. Moreover, in reality, atoms behave in a quantum mechanical manner and the reaction might be successful to form the product even though the energy of the reactants is not enough to overcome the activation energy via quantum tunnelling. Moreover, in reality, the transition state is not necessarily at the lowest saddle point at high temperatures. Thus, there are alternative pathway to the reaction.&lt;br /&gt;
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As a result, the predicted reaction rate values by using Transition State Theory would be lower than the experimental values due to limitations of the assumptions.&lt;br /&gt;
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{{fontcolor|pink| You are very close to the right idea in point 3 but you haven&#039;t quite followed the thought through to completion. This assumption (point 3) means that TST does not account for the idea of barrier recrossing. I.e. in TST once a molecule has hit the TS, that&#039;s it, the reaction is successful. In reality, the molecule can go back to the reactants side, and then over the TS to the product side, and dance around over the TS for a bit. This means that TST predicts that the rate from TST would be higher than in real life (reaction occurs quicker) as it doesn&#039;t account for this extra time spent at the TS. So TST overpredicts the rate constant. &lt;br /&gt;
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Also note that tunelling is not accounted for in this experiment, and also tunneling would accelerate the reaction relative to theoretical prediction (no tunneling) and therefore would have the opposite effect to the barrier recrossing scenario. [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:22, 28 May 2019 (BST)}}&lt;br /&gt;
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== Exercise 2 : F - H - H system ==&lt;br /&gt;
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=== PES inspection ===&lt;br /&gt;
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[[File:JEL3117_F_HH_potential_curve1.png|frame|none|Figure 14. the potential energy surface of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
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[[File:JEL3117_H_HF_potential_curve1.png|frame|none|Figure 15. the potential energy surface of H + HF reaction]]&lt;br /&gt;
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Based on the potential energy surfaces, the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic because the energy of the reactant is higher than the energy of the product and the H + HF reaction is endothermic because the energy of the product is higher than the energy of the reactant.&lt;br /&gt;
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This means that the bond strength of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is weaker than the bond strength of HF because the energy released from breaking H-H bond is lower than the energy required to form the H-F bond for the endothermic F + HF reaction and the energy released from breaking H-F bond is higher than the energy required to form the H-H bond for the exothermic F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction .&lt;br /&gt;
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=== Approximate Position of the transition state ===&lt;br /&gt;
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[[File:JEL3117_F_H2_approximate_TS_intermoleculardistance2.png|frame|none|Figure 16. The intermolecular distance vs time graph of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction]]&lt;br /&gt;
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[[File:JEL3117_F_H2_approximate_TS_potential_surface2.png|frame|none|Figure 17. The potential energy surface of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction indicating the approximate position of the transition state.]]&lt;br /&gt;
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Based on the Hammond&#039;s postulate, the transition state of the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; lies near the reactant. Looking at  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; graph, the transition state therefore lies near the reactant and it is supported by the intermolecular vs time graph as shown above (No change in the intermolecular distances for a subsequent period of time). Likewise, the transition state of the endothermic H + HF reaction lies near the product.&lt;br /&gt;
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With trial and errors, the position of the transition state for the exothermic F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction was found at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;(AB Distance) = 1.8106929 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(BC Distance) = 0.745 Å.&lt;br /&gt;
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The position of the transition state for the endothermic H + HF reaction was found at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;(AB Distance) = 0.745 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(BC Distance) = 1.8106929 Å.&lt;br /&gt;
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The activation energies of both of the reactions were found by displacing the activated complex slightly from the transition state.&lt;br /&gt;
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[[File:JEL_3117_energy_time_graph_exothermic.png|frame|none|Figure 18. Energy vs time graph of the exothermic reaction which illustrates the activation energy of the reaction.]]&lt;br /&gt;
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[[File:JEL_3117_energy_time_graph_endothermic.png|frame|none|Figure 19. Energy vs time graph of the endothermic reaction which illustrates the activation energy of the reaction.]]&lt;br /&gt;
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The activation energy of the exothermic reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; was calculated by displacing r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; to 1.8107 Å. However, the activation energy of the exothermic reaction was negligible such that was hard to be observed from the energy vs time graph.&lt;br /&gt;
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The activation energy of the endothermic reaction was calculated by displacing r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; to 1.8106 Å. The activation energy was found as 29.5 KJ/mol. &lt;br /&gt;
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=== Reaction Dynamics ===&lt;br /&gt;
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By the conservation of energy, the total energy is always conserved. At the start, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and  and F atom are stationary thus they only have potential energies. As they are brought together, the potential energies between them decrease and the kinetic energies of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F atom subsequently increase. As they collide, they start to oscillate and H-H bond is broken and new H-F bond is formed. Since the reaction is exothermic, the excess energy is released from the reaction as heat and the remaining energy is converted to the vibrational energy of HF molecule and kinetic energy of H atom.&lt;br /&gt;
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{{fontcolor|pink|How can the potential energy of the system be decreasing as it goes up the hill of the TS? [[User:Rk2918|Rk2918]] ([[User talk:Rk2918|talk]]) 11:25, 28 May 2019 (BST)}}&lt;br /&gt;
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Experimentally, the above mechanism can be confirmed by measuring the heat released during the reaction with a calorimeter and the vibrational energy of HF molecule can be measured by using IR. &lt;br /&gt;
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[[File:JEL_3117_momentum_time_graph_exothermic.png|frame|none|Figure 19. Energy vs time graph of the endothermic reaction which illustrates the activation energy of the reaction.]]&lt;br /&gt;
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=== Polanyi&#039;s empirical rule ===&lt;br /&gt;
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The position of the transition state is important in determining the distribution of energy between different modes. For the early transition (exothermic reaction), having translational energy in majority is sufficient to form the product because having vibrational energy would cause the molecule to slide the potential energy surface side to side such that it does not have enough energy to overcome the activation energy. However, for the late transition (endothermic reaction, having vibrational energy helps to climb the potential energy surface up to the transition state. Having too much vibrational energy bounces back the product to the reactant.&amp;lt;ref name=&amp;quot;polany&#039;s rule&amp;quot;/&amp;gt;&lt;br /&gt;
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== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;MorsePotential&amp;quot;&amp;gt; Chemistry LibreTexts. &#039;&#039;The Morse Potential graph&#039;&#039;. Available from : https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Map%3A_Physical_Chemistry_(McQuarrie_and_Simon)/05._The_Harmonic_Oscillator_and_the_Rigid_Rotator%3A_Two_Spectroscopic_Models/5.3%3A_The_Harmonic_Oscillator_Approximates_Vibrations &amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;transition state&amp;quot;&amp;gt; &lt;br /&gt;
Atkins, P.W., and Paula J. De. &#039;&#039;Atkin&#039;s Physical Chemistry&#039;&#039;. Oxford: Oxford University Press. 2006&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;polany&#039;s rule&amp;quot;&amp;gt; Jeffrey I.Steinfeld, Joseph S. Francisco, William L.Hase. &#039;&#039;Chemical Kinetics and Dynamics&#039;&#039;. United States: A Paramount Communications Company, 1989 &amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Rk2918</name></author>
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