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	<updated>2026-04-20T21:24:50Z</updated>
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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723772</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723772"/>
		<updated>2018-05-18T16:24:30Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero. &lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the reaction trajectory of the dynamics trajectory but occurs at longer time. The momentum of the MEP trajectory is always zero because the velocity is reset to zero in each time step. Therefore the MEP trajectory is smooth.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! [[File:zy1416_DYNAMICS.png|300px|center]] !! [[File:zy1416_MEP.png|300px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t :&lt;br /&gt;
(500 steps for the dynamics calculation and 100000 steps for the MEP calculation)&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! 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; !! !! 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;
! !! MEP !! Dynamics !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 8.99 || 0.74 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74 || 1.75 || 8.93 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 1.24 || 0 || 2.48&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 2.47 || 0 || 1.26  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
*With the initial conditions of 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;, the r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; values under MEP and dynamics calculations eventually convergence as the H-H bond length is 0.74 Å. The r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; differs because the two trajectories end at different points after the formation of the H-H molecule, in which the hydrogen atom formed is at different positions.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:[1]&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
== EXERCISE 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics=== &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
* Conclusion:  The results agree with the Polanyi&#039;s empirical rules[2], which state that the vibrational energy is more efficient in promoting late-transition-state reactions and the translational energy is more efficient in promoting early-transition-state reactions.  &lt;br /&gt;
&lt;br /&gt;
== Reference ==&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD 3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723751</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723751"/>
		<updated>2018-05-18T16:22:17Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero. &lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the reaction trajectory of the dynamics trajectory but occurs at longer time. The momentum of the MEP trajectory is always zero because the velocity is reset to zero in each time step. Therefore the MEP trajectory is smooth.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! [[File:zy1416_DYNAMICS.png|300px|center]] !! [[File:zy1416_MEP.png|300px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t :&lt;br /&gt;
(500 steps for the dynamics calculation and 100000 steps for the MEP calculation)&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! 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; !! !! 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;
! !! MEP !! Dynamics !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 8.99 || 0.74 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74 || 1.75 || 8.93 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 1.24 || 0 || 2.48&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 2.47 || 0 || 1.26  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
*With the initial conditions of 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;, the r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; values under MEP and dynamics calculations eventually convergence as the H-H bond length is 0.74 Å. The r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; differs because the two trajectories end at different points after the formation of the H-H molecule, in which the hydrogen atom formed is at different positions.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:[1]&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
== EXERCISE 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics=== &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[2], which state that the vibrational energy is more efficient in promoting late-transition-state reactions and the translational energy is more efficient in promoting early-transition-state reactions.  &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
== Reference ==&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD 3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723748</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723748"/>
		<updated>2018-05-18T16:21:50Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero. &lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the reaction trajectory of the dynamics trajectory but occurs at longer time. The momentum of the MEP trajectory is always zero because the velocity is reset to zero in each time step. Therefore the MEP trajectory is smooth.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! [[File:zy1416_DYNAMICS.png|300px|center]] !! [[File:zy1416_MEP.png|300px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t :&lt;br /&gt;
(500 steps for the dynamics calculation and 100000 steps for the MEP calculation)&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! 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; !! !! 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;
! !! MEP !! Dynamics !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 8.99 || 0.74 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74 || 1.75 || 8.93 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 1.24 || 0 || 2.48&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 2.47 || 0 || 1.26  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
With the initial conditions of 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;, the r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; values under MEP and dynamics calculations eventually convergence as the H-H bond length is 0.74 Å. The r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; differs because the two trajectories end at different points after the formation of the H-H molecule, in which the hydrogen atom formed is at different positions.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:[1]&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
== EXERCISE 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics=== &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[2], which state that the vibrational energy is more efficient in promoting late-transition-state reactions and the translational energy is more efficient in promoting early-transition-state reactions.  &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
== Reference ==&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD 3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723736</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723736"/>
		<updated>2018-05-18T16:20:20Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ==&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero. &lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the reaction trajectory of the dynamics trajectory but occurs at longer time. The momentum of the MEP trajectory is always zero because the velocity is reset to zero in each time step. Therefore the MEP trajectory is smooth.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! [[File:zy1416_DYNAMICS.png|300px|center]] !! [[File:zy1416_MEP.png|300px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t :&lt;br /&gt;
(500 steps for the dynamics calculation and 100000 steps for the MEP calculation)&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! 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; !! !! 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;
! !! MEP !! Dynamics !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 8.99 || 0.74 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74 || 1.75 || 8.93 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 1.24 || 0 || 2.48&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 2.47 || 0 || 1.26  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
With the initial conditions of 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;, the r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; values under MEP and dynamics calculations eventually convergence as the H-H bond length is 0.74 Å. The r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; differs because the two trajectories end at different points after the formation of the H-H molecule, in which the hydrogen atom formed is at different positions.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:[1]&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics=== &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[2], which state that the vibrational energy is more efficient in promoting late-transition-state reactions and the translational energy is more efficient in promoting early-transition-state reactions.  &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
== Reference ==&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD 3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723726</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723726"/>
		<updated>2018-05-18T16:18:57Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ==&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero. &lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the reaction trajectory of the dynamics trajectory but occurs at longer time. The momentum of the MEP trajectory is always zero because the velocity is reset to zero in each time step. Therefore the MEP trajectory is smooth.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! [[File:zy1416_DYNAMICS.png|300px|center]] !! [[File:zy1416_MEP.png|300px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t :&lt;br /&gt;
(500 steps for the dynamics calculation and 100000 steps for the MEP calculation)&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! 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; !! !! 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;
! !! MEP !! Dynamics !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 8.99 || 0.74 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74 || 1.75 || 8.93 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 1.24 || 0 || 2.48&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 2.47 || 0 || 1.26  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
With the initial conditions of 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;, the r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; values under MEP and dynamics calculations eventually convergence as the H-H bond length is 0.74 Å. The r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; differs because the two trajectories end at different points after the formation of the H-H molecule, in which the hydrogen atom formed is at different positions.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:[1]&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;PES inspection&#039;&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039;=== &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[2], which state that the vibrational energy is more efficient in promoting late-transition-state reactions and the translational energy is more efficient in promoting early-transition-state reactions.  &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
== Reference ==&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD 3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723717</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723717"/>
		<updated>2018-05-18T16:18:15Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ==&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero. &lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the reaction trajectory of the dynamics trajectory but occurs at longer time. The momentum of the MEP trajectory is always zero because the velocity is reset to zero in each time step. Therefore the MEP trajectory is smooth.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! [[File:zy1416_DYNAMICS.png|300px|center]] !! [[File:zy1416_MEP.png|300px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t :&lt;br /&gt;
(500 steps for the dynamics calculation and 100000 steps for the MEP calculation)&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! 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; !! !! 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;
! !! MEP !! Dynamics !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 8.99 || 0.74 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74 || 1.75 || 8.93 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 1.24 || 0 || 2.48&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 2.47 || 0 || 1.26  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
With the initial conditions of 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, the r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; values under MEP and dynamics calculations eventually convergence as the H-H bond length is 0.74 Å. The r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; differs because the two trajectories end at different points after the formation of the H-H molecule, in which the hydrogen atom formed is at different positions.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:[1]&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;PES inspection&#039;&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039;=== &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[2], which state that the vibrational energy is more efficient in promoting late-transition-state reactions and the translational energy is more efficient in promoting early-transition-state reactions.  &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
== Reference ==&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD 3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723706</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723706"/>
		<updated>2018-05-18T16:17:13Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero. &lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the reaction trajectory of the dynamics trajectory but occurs at longer time. The momentum of the MEP trajectory is always zero because the velocity is reset to zero in each time step. Therefore the MEP trajectory is smooth.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! [[File:zy1416_DYNAMICS.png|300px|center]] !! [[File:zy1416_MEP.png|300px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t :&lt;br /&gt;
(500 steps for the dynamics calculation and 100000 steps for the MEP calculation)&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! 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; !! !! 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;
! !! MEP !! Dynamics !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 8.99 || 0.74 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74 || 1.75 || 8.93 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 1.24 || 0 || 2.48&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 2.47 || 0 || 1.26  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
With the initial conditions of 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, the r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; values under MEP and dynamics calculations eventually convergence as the H-H bond length is 0.74 Å. The r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; differs because the two trajectories end at different points after the formation of the H-H molecule, in which the hydrogen atom formed is at different positions.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:[1]&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[2], which state that the vibrational energy is more efficient in promoting late-transition-state reactions and the translational energy is more efficient in promoting early-transition-state reactions.  &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
=== Reference ===&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD 3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723680</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723680"/>
		<updated>2018-05-18T16:14:26Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero. &lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the reaction trajectory of the dynamics trajectory but occurs at longer time. The momenta of the MEP trajectory is always zero because the velocity is reset to zero in each time step. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! [[File:zy1416_DYNAMICS.png|300px|center]] !! [[File:zy1416_MEP.png|300px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t :&lt;br /&gt;
(500 steps for the dynamics calculation and 100000 steps for the MEP calculation)&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! 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; !! !! 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;
! !! MEP !! Dynamics !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 8.99 || 0.74 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74 || 1.75 || 8.93 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 1.24 || 0 || 2.48&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 2.47 || 0 || 1.26  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
With the initial conditions of 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, the r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; values under MEP and dynamics calculations eventually convergence as the H-H bond length is 0.74 Å. The r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; differs because the two trajectories end at different points after the formation of the H-H molecule, in which the hydrogen atom formed is at different positions.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:[1]&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[2], which state that the vibrational energy is more efficient in promoting late-transition-state reactions and the translational energy is more efficient in promoting early-transition-state reactions.  &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
=== Reference ===&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD 3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_MEP.png&amp;diff=723673</id>
		<title>File:Zy1416 MEP.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_MEP.png&amp;diff=723673"/>
		<updated>2018-05-18T16:13:58Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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		<title>File:Zy1416 DYNAMICS.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_DYNAMICS.png&amp;diff=723654"/>
		<updated>2018-05-18T16:11:43Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723535</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723535"/>
		<updated>2018-05-18T15:58:59Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the reaction trajectory of the dynamics trajectory but occurs at longer time. The momenta of the MEP trajectory is always zero because the velocity is reset to zero in each time step. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t :&lt;br /&gt;
(500 steps for the dynamics calculation and 100000 steps for the MEP calculation)&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! 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; !! !! 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;
! !! MEP !! Dynamics !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 8.99 || 0.74 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74 || 1.75 || 8.93 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 1.24 || 0 || 2.48&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 2.47 || 0 || 1.26  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
With the initial conditions of 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, the r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; values under MEP and dynamics calculations eventually convergence as the H-H bond length is 0.74 Å. The r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; differs because the two trajectories end at different points after the formation of the H-H molecule, in which the hydrogen atom formed is at different positions.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:[1]&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[2], which state that the vibrational energy is more efficient in promoting late-transition-state reactions and the translational energy is more efficient in promoting early-transition-state reactions.  &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
=== Reference ===&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD 3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723329</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723329"/>
		<updated>2018-05-18T15:33:09Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the reaction trajectory of the dynamics trajectory but occurs at longer time. The momenta of the MEP trajectory is always zero because the velocity is reset to zero in each time step. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_momenta_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! r1 = rts+δ, r2 = rts !! !! r1 = rts+δ, r2 = rts !!&lt;br /&gt;
|-&lt;br /&gt;
! !! MEP !! Dynamics !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; values under MEP and dynamics calculations eventually convergence&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:[1]&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[2], which state that the vibrational energy is more efficient in promoting late-transition-state reactions and the translational energy is more efficient in promoting early-transition-state reactions.  &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
=== Reference ===&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD 3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723323</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723323"/>
		<updated>2018-05-18T15:32:38Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the reaction trajectory of the dynamics trajectory but occurs at longer time. The momenta of the MEP trajectory is always zero because the velocity is reset to zero in each time step. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_momenta_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! r1 = rts+δ, r2 = rts !! !! r1 = rts+δ, r2 = rts !!&lt;br /&gt;
|-&lt;br /&gt;
! !! MEP !! Dynamics !! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; values under MEP and dynamics calculations eventually convergence&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:[1]&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[2], which state that the vibrational energy is more efficient in promoting late-transition-state reactions and the translational energy is more efficient in promoting early-transition-state reactions.  &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
=== Reference ===&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD 3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723076</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=723076"/>
		<updated>2018-05-18T15:06:04Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_momenta_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:[1]&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[2], which state that the vibrational energy is more efficient in promoting late-transition-state reactions and the translational energy is more efficient in promoting early-transition-state reactions.  &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
=== Reference ===&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722910</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722910"/>
		<updated>2018-05-18T14:45:57Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_momenta_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[1], which state that the vibrational energy is more efficient &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
=== Reference ===&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722892</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722892"/>
		<updated>2018-05-18T14:43:37Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_momenta_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[1], which state that &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
=== Reference ===&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722889</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722889"/>
		<updated>2018-05-18T14:43:23Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_momenta_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[1], which state that &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|500px|center]]&lt;br /&gt;
&lt;br /&gt;
=== Reference ===&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722886</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722886"/>
		<updated>2018-05-18T14:42:48Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_momenta_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|350px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The procedure described is illustrated in the following animation snapshots. After the collision, the large momentum that the reactant hydrogen atom contains is still large.As a result, even if an H-H bond can be formed, it would immediately be broken due to an excess vibrational energy between two atoms. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products. By comparing this condition to the initial condition, the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;, which is the translational kinetic energy of the H atom, is reduced by a half; and the p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;, the vibrational energy of the H-F bond is increased to -0.5. This indicates that the vibrational energy has a greater contribution to the feasibility of the reaction than the translational energy. This is the opposite situation of the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F reaction.&lt;br /&gt;
&lt;br /&gt;
The results agree with the Polanyi&#039;s empirical rules[1], which state that &lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;br /&gt;
&lt;br /&gt;
=== Reference ===&lt;br /&gt;
1.Zhang, Z., Zhou, Y., Zhang, D., Czakó, G. &amp;amp; Bowman, J. Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction. The Journal of Physical Chemistry Letters 3, 3416-3419 (2012).&lt;br /&gt;
2.Bligaard, T. &amp;amp; Nørskov, J. Heterogeneous Catalysis. Chemical Bonding at Surfaces and Interfaces 255-321 (2008). doi:10.1016/b978-044452837-7.50005-8&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722654</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722654"/>
		<updated>2018-05-18T14:21:02Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_momenta_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1, the reaction now becomes successful. It indicates that the F-H vibration energy has a larger contribution for the feasibility of this reaction compared to the translational energy which is the kinetic energy of the hydrogen atom which is defined by the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;&lt;br /&gt;
[[File:zy1416_Minus0.8.png|400px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722630</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722630"/>
		<updated>2018-05-18T14:18:17Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_momenta_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1.&lt;br /&gt;
[[File:zy1416_Minus0.8.png|200px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722624</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722624"/>
		<updated>2018-05-18T14:17:30Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for a few values of momenta such as +2.6 and -2.4. The feasibility of the reaction is not solely dependent on the energy distribution, but might also rely on the proceeding of the trajectory which would be very sensitive to specific conditions. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
When the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; is increased slightly from -0.5 to -0.8 with p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; being only 0.1.&lt;br /&gt;
[[File:zy1416_Minus0.8.png|200px|center]] &lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_Minus0.8.png&amp;diff=722620</id>
		<title>File:Zy1416 Minus0.8.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_Minus0.8.png&amp;diff=722620"/>
		<updated>2018-05-18T14:17:19Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722520</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722520"/>
		<updated>2018-05-18T14:09:02Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for very few values of momenta.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! {{fontcolor|blue|p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;}} !! {{fontcolor|blue|Contour Plot}}&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|blue|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|blue|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722509</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722509"/>
		<updated>2018-05-18T14:08:17Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for very few values of momenta.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot &lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || {{fontcolor|red|-2.4}} || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || {{fontcolor|red|2.6}} || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722486</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722486"/>
		<updated>2018-05-18T14:06:12Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for very few values of momenta.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot &lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || -2.4 || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 2.6 || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722479</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722479"/>
		<updated>2018-05-18T14:05:21Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With a small momentum of -0.5 for the coming H atom, the reaction would be mostly unsuccessful even the H-H bond has a vibration energy which is significantly larger than the activation energy (0.255 kcal/mol) except for very few values of momenta.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot &lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]] || -2.4 || [[File:zy1416_minus2.4.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]] || [[File:Zy1416_2.6.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_2.6.png&amp;diff=722471</id>
		<title>File:Zy1416 2.6.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_2.6.png&amp;diff=722471"/>
		<updated>2018-05-18T14:04:48Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: Zy1416 uploaded a new version of File:Zy1416 2.6.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_minus2.4.png&amp;diff=722464</id>
		<title>File:Zy1416 minus2.4.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_minus2.4.png&amp;diff=722464"/>
		<updated>2018-05-18T14:03:38Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_2.6.png&amp;diff=722460</id>
		<title>File:Zy1416 2.6.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_2.6.png&amp;diff=722460"/>
		<updated>2018-05-18T14:03:16Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722362</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722362"/>
		<updated>2018-05-18T13:49:44Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722357</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722357"/>
		<updated>2018-05-18T13:48:52Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|200px|center]] || -2.9 || [[File:zy1416_minus2.9.png|200px|center]] || -2.0 || [[File:zy1416_minus2.0.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|200px|center]] || 0.0 || [[File:zy1416_0.png|200px|center]] || 1.0 || [[File:zy1416_minus1.0.png|200px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|200px|center]] || 2.9 || [[File:zy1416_2.9.png|200px|center]] || 3.0 || [[File:zy1416_3.0.png|200px|center]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722350</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722350"/>
		<updated>2018-05-18T13:48:12Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot&lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|250px|center]] || -2.9 || [[File:zy1416_minus2.9.png|250px|center]] || -2.0 || [[File:zy1416_minus2.0.png|250px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|250px|center]] || 0.0 || [[File:zy1416_0.png|250px|center]] || 1.0 || [[File:zy1416_minus1.0.png|250px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|250px|center]] || 2.9 || [[File:zy1416_2.9.png|250px|center]] || 3.0 || [[File:zy1416_3.0.png|250px|center]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722332</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722332"/>
		<updated>2018-05-18T13:45:16Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot !!  p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot &lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png|250px|center]] || 3.0 || [[File:zy1416_3.0.png|250px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -2.9 || [[File:zy1416_minus2.9.png|250px|center]] || 2.9 || [[File:zy1416_2.9.png|250px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.0 || [[File:zy1416_minus2.0.png|250px|center]] || 2.0 || [[File:zy1416_2.0.png|250px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|250px|center]] || 1.0 || [[File:zy1416_1.0.png|250px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -0.0 || [[File:zy1416_0.png|250px|center]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722318</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=722318"/>
		<updated>2018-05-18T13:42:53Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; in the potential energy surface at one minimum is zero and the gradient of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; in another minimum is zero.&lt;br /&gt;
&lt;br /&gt;
The curvatures of both components of the potential energy surface for minima are positive. i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0 ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. But one of the curvatures is negative and one of the curvatures is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! Contour Plot &lt;br /&gt;
|-&lt;br /&gt;
| -3.0 || [[File:minus3.0_zy1416.png.png|250px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.9 || [[File:zy1416_minus2.9.png|250px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -2.0 || [[File:zy1416_minus2.0.png|250px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.0 || [[File:zy1416_minus1.0.png|250px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -0.0 || [[File:zy1416_0.png|250px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| 1.0 || [[File:zy1416_1.0.png|250px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| 2.0 || [[File:zy1416_2.0.png|250px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| 2.9 || [[File:zy1416_2.9.png|250px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| 3.0 || [[File:zy1416_3.0.png|250px|center]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_3.0.png&amp;diff=722317</id>
		<title>File:Zy1416 3.0.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_3.0.png&amp;diff=722317"/>
		<updated>2018-05-18T13:42:42Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_0.png&amp;diff=722310</id>
		<title>File:Zy1416 0.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_0.png&amp;diff=722310"/>
		<updated>2018-05-18T13:41:53Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_2.9.png&amp;diff=722298</id>
		<title>File:Zy1416 2.9.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_2.9.png&amp;diff=722298"/>
		<updated>2018-05-18T13:40:38Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_2.0.png&amp;diff=722295</id>
		<title>File:Zy1416 2.0.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_2.0.png&amp;diff=722295"/>
		<updated>2018-05-18T13:40:18Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_1.0.png&amp;diff=722293</id>
		<title>File:Zy1416 1.0.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_1.0.png&amp;diff=722293"/>
		<updated>2018-05-18T13:39:57Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_minus1.0.png&amp;diff=722287</id>
		<title>File:Zy1416 minus1.0.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_minus1.0.png&amp;diff=722287"/>
		<updated>2018-05-18T13:39:35Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_minus2.0.png&amp;diff=722282</id>
		<title>File:Zy1416 minus2.0.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_minus2.0.png&amp;diff=722282"/>
		<updated>2018-05-18T13:39:16Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_minus2.9.png&amp;diff=722276</id>
		<title>File:Zy1416 minus2.9.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_minus2.9.png&amp;diff=722276"/>
		<updated>2018-05-18T13:38:47Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Minus3.0_zy1416.png&amp;diff=722268</id>
		<title>File:Minus3.0 zy1416.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Minus3.0_zy1416.png&amp;diff=722268"/>
		<updated>2018-05-18T13:38:09Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=721319</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=721319"/>
		<updated>2018-05-17T21:36:18Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r2 in the potential energy surface at one minimum and the gradient of r1 in another minimum.&lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. &lt;br /&gt;
&lt;br /&gt;
The curvatures of the potential energy surface for minima are positive&lt;br /&gt;
&lt;br /&gt;
i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;=∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
&lt;br /&gt;
At the transition states, one of the curvature is negative and one of the curvature is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;PES inspection&#039;&#039;&#039; &lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! 0.1(p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=-0.8) !! 0.1 &lt;br /&gt;
|-&lt;br /&gt;
| Contour Plot || [[File:zy1416_Reducingoverall.png|300px|center]] || [[File:zy1416_0.1.png|300px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| Feasibility || reactive || reactive  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
reactive 2.90 2.94 2.95 2.89 2.87 2.86 2.85 2.84 2.83 2.82 2.81 2.79 2.78 2.77 2.73 2.72&lt;br /&gt;
unreactive 3.00 2.99 2.98 2.97 2.96 2.93 2.92 2.91 2.88 2.80 2.76 2.75 2.74 2.71 2.70&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=721316</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=721316"/>
		<updated>2018-05-17T21:35:41Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r2 in the potential energy surface at one minimum and the gradient of r1 in another minimum.&lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. &lt;br /&gt;
&lt;br /&gt;
The curvatures of the potential energy surface for minima are positive&lt;br /&gt;
&lt;br /&gt;
i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;=∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
&lt;br /&gt;
At the transition states, one of the curvature is negative and one of the curvature is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;PES inspection&#039;&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Reaction Dynamics&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! 0.1(p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=-0.8) !! 0.1 &lt;br /&gt;
|-&lt;br /&gt;
| Contour Plot || [[File:zy1416_Reducingoverall.png|300px|center]] || [[File:zy1416_0.1.png|300px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| Feasibility || reactive || reactive  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
reactive 2.90 2.94 2.95 2.89 2.87 2.86 2.85 2.84 2.83 2.82 2.81 2.79 2.78 2.77 2.73 2.72&lt;br /&gt;
unreactive 3.00 2.99 2.98 2.97 2.96 2.93 2.92 2.91 2.88 2.80 2.76 2.75 2.74 2.71 2.70&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=721311</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=721311"/>
		<updated>2018-05-17T21:34:12Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r2 in the potential energy surface at one minimum and the gradient of r1 in another minimum.&lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. &lt;br /&gt;
&lt;br /&gt;
The curvatures of the potential energy surface for minima are positive&lt;br /&gt;
&lt;br /&gt;
i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;=∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
&lt;br /&gt;
At the transition states, one of the curvature is negative and one of the curvature is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;PES inspection&#039;&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! 0.1(p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=-0.8) !! 0.1 &lt;br /&gt;
|-&lt;br /&gt;
| Contour Plot || [[File:zy1416_Reducingoverall.png|300px|center]] || [[File:zy1416_0.1.png|300px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| Feasibility || reactive || reactive  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
reactive 2.90 2.94 2.95 2.89 2.87 2.86 2.85 2.84 2.83 2.82 2.81 2.79 2.78 2.77 2.73 2.72&lt;br /&gt;
unreactive 3.00 2.99 2.98 2.97 2.96 2.93 2.92 2.91 2.88 2.80 2.76 2.75 2.74 2.71 2.70&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:ZY14166_HFF_REACTIVE.png‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:ZY14166_HFF_REACTIVE.png&amp;diff=721310</id>
		<title>File:ZY14166 HFF REACTIVE.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:ZY14166_HFF_REACTIVE.png&amp;diff=721310"/>
		<updated>2018-05-17T21:33:59Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=721306</id>
		<title>MRD:zy1416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:zy1416&amp;diff=721306"/>
		<updated>2018-05-17T21:32:37Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Molecular reaction dynamics&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 1:&#039;&#039;&#039; &#039;&#039;&#039;What value do the different components of the gradient of the potential energy surface have at a minimum and at a transition structure? Briefly explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The gradients of r2 in the potential energy surface at one minimum and the gradient of r1 in another minimum.&lt;br /&gt;
 &lt;br /&gt;
At the transition state, the gradients for both components are both zero. &lt;br /&gt;
&lt;br /&gt;
The curvatures of the potential energy surface for minima are positive&lt;br /&gt;
&lt;br /&gt;
i.e the second derivative ∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r1)/∂(r1)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;=∂&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;V(r2)/∂(r2)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; =&amp;gt; 0  &lt;br /&gt;
&lt;br /&gt;
At the transition states, one of the curvature is negative and one of the curvature is positive.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Question 2: Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039; &#039;&#039;&#039;&amp;lt;nowiki/&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
* The transition state position is estimated at r1=r2= 0.908 Å. The “Internuclear Distances vs Time” plot shows two almost flat lines, indicating that the atoms hardly oscillates and are close to an equilibrium. The distance of AB equals to the distance of BC so the two lines overlap.&lt;br /&gt;
[[File:Zy1416_transiton_state_estimate.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 3: Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
* The MEP trajectory reflects the initial part of the dynamics trajectory but occurs at larger time scale. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! distance &lt;br /&gt;
| [[File:Mep_distance_zy1416.png|300px|center]]  || [[File:Dynamics_distance_zy1416.png|300px|left]]&lt;br /&gt;
|-&lt;br /&gt;
! momenta &lt;br /&gt;
| [[File:Mep_momenta_zy1416.png|300px|left]]  || [[File:Dynamics_distance_zy1416.png|300px|left]] &lt;br /&gt;
|}&lt;br /&gt;
* Final values of the positions r1(t) r2(t) and the average momenta  p1(t) p2(t) at large t:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
! !! MEP !! Dynamics&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &lt;br /&gt;
| 1.72 || 2.76 &lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0.75 || 0.74&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
! &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  &lt;br /&gt;
| 2.47 || 1.26&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 4: Complete the table by adding a column with the total energy, and another column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a plot of the trajectory and a small description for what happens along the trajectory.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&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&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! reactivity !! plot !! description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.-018 || reactive || [[File:zy1416_Trajectory_1.png|300px|center]] || trajectory crosses the TS and moves towards the product; r2 decreases in the entrance channel and r1 does not fluctuate; trajectory shows vibration in r2 as r1 increases in the exit channel  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || unreactive || [[File:zy1416_Trajectory_2.png|300px|center]] || trajectory does not reach the transition state and moves back towards the initial point in the entrance channel; shows vibration in r1&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || reactive || [[File:zy1416_Trajectory_3.png|300px|center]] || trajectory crosses the TS and moves towards the product; slight vibration in r1 as r2 decreases in the entrance channel; vibration in r2 as r1 increases in the exit channel &lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || unreactive || [[File:zy1416_Trajectory_4.png|300px|center]] || trajectory crosses the transition state region but reverts back to the reactants&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || reactive || [[File:zy1416_Trajectory_5.png|300px|center]] || trajectory crosses the transition state and reverts back to the entrance channel and eventually moves towards the products&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
* There are three main assumptions made in the transition state theory:&lt;br /&gt;
1.The quantum-tunneling effects and the Born-Oppenheimer approximation are ignored. &lt;br /&gt;
&lt;br /&gt;
2.The atoms in the reactant state have energies that are Boltzmann distributed.&lt;br /&gt;
&lt;br /&gt;
3.At the transition state, with a velocity towards the product configuration, it will not re-enter the initial state region again.&lt;br /&gt;
* The limitation of the transition state theory is that the quantum-tunneling effect is assumed to be negligible. However, quantum mechanics shows that particles can tunnel through the energy barrier created by the transition state, allowing the reaction to occur. So the experimental values of the reaction rate would be higher than the theoretical values.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;EXERCISE 2: F - H - H system&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;PES inspection&#039;&#039;&#039; ===&lt;br /&gt;
&#039;&#039;&#039;Question 6: Classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;H + HF :&#039;&#039;&#039;&lt;br /&gt;
[[File:zy1416_Surface_Plot_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
It can be seen from the PES plot of this reaction that the products have higher energy than the reactants, indicating an endothermic reaction.&lt;br /&gt;
H-F bond is strongly polarisd and has a large ionic component with strong bond strength. The energy required for breaking the H-F bond can not be compensated by the energy gain from the formation of a H-H bond. So overall the reaction is endothermic.   &lt;br /&gt;
* &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:&#039;&#039;&#039; &lt;br /&gt;
[[File:zy1416_Surface_Plot_HHF.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
The PES plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows that the reactants have higher energy than the products. This reaction is exothermic. As discussed above, the formation of H-F bond would gain a large enthalpy due to strong bond strength and this energy gain compensates the energy lose for breaking the H-H bond. The overall reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt; &#039;&#039;&#039;Question 7: Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* For H+HF, the reaction is endothermic and the transition state would resemble the product; for the other reaction which is exothermic, the transition state would resemble the reactants which is the products for the first reaction. These two reactions would have the same transition state H--H--F. And the approximate position can be located on the PES plot.&lt;br /&gt;
&lt;br /&gt;
[[File:zy1416_Surface_Plot_transition_state.png|500px|center]]&lt;br /&gt;
* The distance between H and H is determined to be 0.745 Å and the distance between H and F is determined to be 1.810 Å. The “Internuclear Distances vs Time” plot confirmed this position. The activation energy for the endothermic reaction is much higher than the exothermic reaction. Because the transition state resembles the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F species and they have similar energies.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_Transition_state_distance.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 8: Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! H+HF !! H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F&lt;br /&gt;
|-&lt;br /&gt;
| [[File:Zy1416_HHF_Ea.png|300px|center]] || [[File:zy1416_H2F_Ea.png|300px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| Ea = (-103.785)-(-134.016) = 30.231 kcal/mol || Ea = (-103.752)-(-104.007) = 0.255 kcal/mol &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Question 9: In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial conditions have been set to be r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=0.74 Å , r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=2.00 Å and momentum&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=-10. The potential energy released is converted into the kinetic energy of the hydrogen atom. It can be seen from the Momenta vs Time plot that p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; increases after the collision. The kinetic energy would be further convert into thermal energy as the product hydrogen atoms collide with each other. There would be an temperature increase for this exothermic reaction which can be measured experimentally. &lt;br /&gt;
&lt;br /&gt;
[[File:ZZy1416_Momenta_H2F.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;br&amp;gt;&#039;&#039;&#039;Questin 10:  Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
* &#039;&#039;&#039;F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; !! 0.1(p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt;=-0.8) !! 0.1 &lt;br /&gt;
|-&lt;br /&gt;
| Contour Plot || [[File:zy1416_Reducingoverall.png|300px|center]] || [[File:zy1416_0.1.png|300px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| Feasibility || reactive || reactive  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
reactive 2.90 2.94 2.95 2.89 2.87 2.86 2.85 2.84 2.83 2.82 2.81 2.79 2.78 2.77 2.73 2.72&lt;br /&gt;
unreactive 3.00 2.99 2.98 2.97 2.96 2.93 2.92 2.91 2.88 2.80 2.76 2.75 2.74 2.71 2.70&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;&#039;H+HF&#039;&#039;&#039;&lt;br /&gt;
When the p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; has a large value above the activation energy (30.231 kcal/mol), which was set to be -20. The hydrogen atom collides with the HF molecule and breaks the H-F bond. However, two hydrogen atoms moves apart and do not form a H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule. The reaction is illustrated in the following animation snapshots.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! [[File:zy1416_HFF_unreactive_animation_0.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_1.png|300px|center]] !! [[File:zy1416_HFF_unreactive_animation_2.png|300px|center]]  &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
One reactive trajectory has the conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 0.91 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0 Å, p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.5 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -10. The trajectory recrosses the transition state region twice and eventually moves into exit channel, forming products.&lt;br /&gt;
&lt;br /&gt;
[[File:Zy1416_HFF_REACTIVE.png ‎|400px|left]]&lt;/div&gt;</summary>
		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_HFF_unreactive_animation_2.png&amp;diff=721305</id>
		<title>File:Zy1416 HFF unreactive animation 2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_HFF_unreactive_animation_2.png&amp;diff=721305"/>
		<updated>2018-05-17T21:32:35Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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		<author><name>Zy1416</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_HFF_unreactive_animation_1.png&amp;diff=721303</id>
		<title>File:Zy1416 HFF unreactive animation 1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Zy1416_HFF_unreactive_animation_1.png&amp;diff=721303"/>
		<updated>2018-05-17T21:32:21Z</updated>

		<summary type="html">&lt;p&gt;Zy1416: &lt;/p&gt;
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		<author><name>Zy1416</name></author>
	</entry>
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