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	<id>https://chemwiki.ch.ic.ac.uk/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=Hys116</id>
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	<updated>2026-04-04T01:18:40Z</updated>
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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722658</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722658"/>
		<updated>2018-05-18T14:21:32Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* F + H2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465 Å&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095 Å&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 Å in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 Å is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.989 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.989) = 0.238 kcal/mol&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 Å is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Graphs of momentum vs time and energy vs time are shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]][[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The momentum graph shows that before the collision, that H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (BC) has kinetic energy as shown by the oscillations in the graph. After the collision, the line for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is transferred to HF. &lt;br /&gt;
This is supported by the energy v time graph which shows that potential and kinetic energy are mirror images, showing that all kinetic energy is converted into potential and vice versa; energy is conserved.&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by analysing the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful.&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful&lt;br /&gt;
&lt;br /&gt;
For p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -3:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
For p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = +3:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is because the excess vibrational energy causes the trajectory to recross the transition state and results in a non-reactive collision.&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722657</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722657"/>
		<updated>2018-05-18T14:21:19Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* HF + H */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465 Å&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095 Å&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 Å in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.989 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.989) = 0.238 kcal/mol&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 Å is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Graphs of momentum vs time and energy vs time are shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]][[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The momentum graph shows that before the collision, that H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (BC) has kinetic energy as shown by the oscillations in the graph. After the collision, the line for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is transferred to HF. &lt;br /&gt;
This is supported by the energy v time graph which shows that potential and kinetic energy are mirror images, showing that all kinetic energy is converted into potential and vice versa; energy is conserved.&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by analysing the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful.&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful&lt;br /&gt;
&lt;br /&gt;
For p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -3:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
For p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = +3:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is because the excess vibrational energy causes the trajectory to recross the transition state and results in a non-reactive collision.&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722643</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722643"/>
		<updated>2018-05-18T14:19:50Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* F + H2: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465 Å&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095 Å&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 Å in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.989 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.989) = 0.238 kcal/mol&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Graphs of momentum vs time and energy vs time are shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]][[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The momentum graph shows that before the collision, that H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (BC) has kinetic energy as shown by the oscillations in the graph. After the collision, the line for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is transferred to HF. &lt;br /&gt;
This is supported by the energy v time graph which shows that potential and kinetic energy are mirror images, showing that all kinetic energy is converted into potential and vice versa; energy is conserved.&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by analysing the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful.&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful&lt;br /&gt;
&lt;br /&gt;
For p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -3:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
For p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = +3:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is because the excess vibrational energy causes the trajectory to recross the transition state and results in a non-reactive collision.&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722634</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722634"/>
		<updated>2018-05-18T14:18:30Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* F + H2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465 Å&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095 Å&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 Å in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.989 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.989) = 0.238 kcal/mol&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Graphs of momentum vs time and energy vs time are shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]][[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The momentum graph shows that before the collision, that H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (BC) has kinetic energy as shown by the oscillations in the graph. After the collision, the line for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is transferred to HF. &lt;br /&gt;
This is supported by the energy v time graph which shows that potential and kinetic energy are mirror images, showing that all kinetic energy is converted into potential and vice versa; energy is conserved.&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by analysing the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful.&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is because the excess vibrational energy causes the trajectory to recross the transition state and results in a non-reactive collision.&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722561</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722561"/>
		<updated>2018-05-18T14:12:01Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* F + H2: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465 Å&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095 Å&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 Å in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01 kcal/mol&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Graphs of momentum vs time and energy vs time are shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]][[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The momentum graph shows that before the collision, that H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (BC) has kinetic energy as shown by the oscillations in the graph. After the collision, the line for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is transferred to HF. &lt;br /&gt;
This is supported by the energy v time graph which shows that potential and kinetic energy are mirror images, showing that all kinetic energy is converted into potential and vice versa; energy is conserved.&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by analysing the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful.&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is because the excess vibrational energy causes the trajectory to recross the transition state and results in a non-reactive collision.&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722551</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722551"/>
		<updated>2018-05-18T14:10:59Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Activation Energies */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465 Å&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095 Å&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 Å in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01 kcal/mol&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Graphs of momentum vs time and energy vs time are shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]][[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The momentum graph shows that before the collision, that H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (BC) has kinetic energy as shown by the oscillations in the graph. After the collision, the line for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is transferred to HF. &lt;br /&gt;
This is supported by the energy v time graph which shows that potential and kinetic energy are mirror images, showing that all kinetic energy is converted into potential and vice versa; energy is conserved.&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by analysing the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful.&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722528</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722528"/>
		<updated>2018-05-18T14:09:30Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Transition State */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465 Å&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095 Å&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Graphs of momentum vs time and energy vs time are shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]][[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The momentum graph shows that before the collision, that H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (BC) has kinetic energy as shown by the oscillations in the graph. After the collision, the line for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is transferred to HF. &lt;br /&gt;
This is supported by the energy v time graph which shows that potential and kinetic energy are mirror images, showing that all kinetic energy is converted into potential and vice versa; energy is conserved.&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by analysing the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful.&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex1_trajectory1.png&amp;diff=722356</id>
		<title>File:Hys ex1 trajectory1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex1_trajectory1.png&amp;diff=722356"/>
		<updated>2018-05-18T13:48:49Z</updated>

		<summary type="html">&lt;p&gt;Hys116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722353</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722353"/>
		<updated>2018-05-18T13:48:32Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Calculating the Reaction Path */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Graphs of momentum vs time and energy vs time are shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]][[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The momentum graph shows that before the collision, that H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (BC) has kinetic energy as shown by the oscillations in the graph. After the collision, the line for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is transferred to HF. &lt;br /&gt;
This is supported by the energy v time graph which shows that potential and kinetic energy are mirror images, showing that all kinetic energy is converted into potential and vice versa; energy is conserved.&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by analysing the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful.&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722323</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722323"/>
		<updated>2018-05-18T13:43:25Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Internuclear distance and momenta at large t */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Graphs of momentum vs time and energy vs time are shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]][[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The momentum graph shows that before the collision, that H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (BC) has kinetic energy as shown by the oscillations in the graph. After the collision, the line for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is transferred to HF. &lt;br /&gt;
This is supported by the energy v time graph which shows that potential and kinetic energy are mirror images, showing that all kinetic energy is converted into potential and vice versa; energy is conserved.&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by analysing the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful.&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722274</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722274"/>
		<updated>2018-05-18T13:38:39Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* F + H2: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|400px]][[File:hys_ex1_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|400px]][[File:hys_ex1_mvtrev.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Graphs of momentum vs time and energy vs time are shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]][[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The momentum graph shows that before the collision, that H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (BC) has kinetic energy as shown by the oscillations in the graph. After the collision, the line for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is transferred to HF. &lt;br /&gt;
This is supported by the energy v time graph which shows that potential and kinetic energy are mirror images, showing that all kinetic energy is converted into potential and vice versa; energy is conserved.&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by analysing the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful.&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722270</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722270"/>
		<updated>2018-05-18T13:38:24Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Polanyi&amp;#039;s empirical rules */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|400px]][[File:hys_ex1_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|400px]][[File:hys_ex1_mvtrev.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Graphs of momentum vs time and energy vs time are shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]][[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The momentum graph shows that before the collision, that H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (BC) has kinetic energy as shown by the oscillations in the graph. After the collision, the line for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is transferred to HF. &lt;br /&gt;
This is supported by the energy v time graph which shows that potential and kinetic energy are mirror images, showing that all kinetic energy is converted into potential and vice versa; energy is conserved.&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by analysing the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful.&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722230</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722230"/>
		<updated>2018-05-18T13:35:14Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|400px]][[File:hys_ex1_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|400px]][[File:hys_ex1_mvtrev.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Graphs of momentum vs time and energy vs time are shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]][[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The momentum graph shows that before the collision, that H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (BC) has kinetic energy as shown by the oscillations in the graph. After the collision, the line for H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is transferred to HF. &lt;br /&gt;
This is supported by the energy v time graph which shows that potential and kinetic energy are mirror images, showing that all kinetic energy is converted into potential and vice versa; energy is conserved.&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by analysing the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722170</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722170"/>
		<updated>2018-05-18T13:28:12Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Reaction Energy */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|400px]][[File:hys_ex1_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|400px]][[File:hys_ex1_mvtrev.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, then recrosses the barrier and collides with other H then crosses the barrier again to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722158</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722158"/>
		<updated>2018-05-18T13:26:30Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* HF + H */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|400px]][[File:hys_ex1_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|400px]][[File:hys_ex1_mvtrev.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]][[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722152</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722152"/>
		<updated>2018-05-18T13:25:50Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Activation Energies */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|400px]][[File:hys_ex1_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|400px]][[File:hys_ex1_mvtrev.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
 &lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722147</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722147"/>
		<updated>2018-05-18T13:25:16Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* HF + H= */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|400px]][[File:hys_ex1_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|400px]][[File:hys_ex1_mvtrev.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01&lt;br /&gt;
&lt;br /&gt;
=====HF + H=====&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722091</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722091"/>
		<updated>2018-05-18T13:18:30Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Activation Energies */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|400px]][[File:hys_ex1_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|400px]][[File:hys_ex1_mvtrev.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 in each direction. &lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; =====&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761&lt;br /&gt;
&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.01&lt;br /&gt;
&lt;br /&gt;
=====HF + H======&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722059</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=722059"/>
		<updated>2018-05-18T13:13:37Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Activation Energies */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|400px]][[File:hys_ex1_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|400px]][[File:hys_ex1_mvtrev.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
The activation energies were calculated by finding the difference between the energy of the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants can be found by displacing the H-F bond length by 0.1 in each direction. &lt;br /&gt;
&lt;br /&gt;
When 0.1 is added, the reaction falls towards the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction. The last point of the trajectory; the beginning of this reaction, can be found and a MEP was plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.752&lt;br /&gt;
Activation energy = -103.751 - (-103.752) = 0.001&lt;br /&gt;
&lt;br /&gt;
Similarly, when 0.1 is subtracted from the H-F bond distance, the reaction falls towards the side of HF + F. Again, the last point of the trajectory was found and a MEP plotted:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Activation energy = -103.751 - (-133.762) = 30.011 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=721064</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=721064"/>
		<updated>2018-05-17T19:20:05Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Reaction Energy */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|400px]][[File:hys_ex1_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|400px]][[File:hys_ex1_mvtrev.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H F momentum: -2&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=721005</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=721005"/>
		<updated>2018-05-17T18:47:42Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* H + H2 System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|400px]][[File:hys_ex1_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|400px]][[File:hys_ex1_mvtrev.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720954</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720954"/>
		<updated>2018-05-17T18:04:07Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* F + H2: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720951</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720951"/>
		<updated>2018-05-17T18:01:56Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* HF + H */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
&lt;br /&gt;
Initial conditions:&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720948</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720948"/>
		<updated>2018-05-17T17:58:18Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Transition State */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]][[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720947</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720947"/>
		<updated>2018-05-17T17:57:33Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Transition State */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
&lt;br /&gt;
H-H distance = 0.7465&lt;br /&gt;
&lt;br /&gt;
H-F distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720944</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720944"/>
		<updated>2018-05-17T17:56:47Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* H + HF ---&amp;gt; + H2 + F */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
&lt;br /&gt;
The surface plot shown below was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720942</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720942"/>
		<updated>2018-05-17T17:56:16Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* F + H2 ---&amp;gt; HF + H */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
&lt;br /&gt;
the following surface plot was produced:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720938</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720938"/>
		<updated>2018-05-17T17:54:09Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Transition State Theory */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: &lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720935</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720935"/>
		<updated>2018-05-17T17:53:54Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Transition State Theory */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures. From the previous examples, the reactions are successful if they have energy equal to or greater than the activation energy so this theory gives accurate predictions for the previous examples.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: &lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720928</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720928"/>
		<updated>2018-05-17T17:51:29Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Reactive and Unreactive Trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: &lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720926</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720926"/>
		<updated>2018-05-17T17:50:40Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Reactive and Unreactive Trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to cross the transition state and break the A-B bond. However there excess momentum so the trajectory recrosses the barrier, resulting in the reformation of the A-B bond and an overall unreactive situation.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the trajectory crossing then recrossing the transition state barrier, however there is still excess momentum so the trajectory crosses the barrier again, resulting in an overall reactive situation.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: &lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720923</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720923"/>
		<updated>2018-05-17T17:47:41Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Reactive and Unreactive Trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum to cross the transition state and for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the trajectory does not cross the transition state and C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to break the A-B bond and draw B towards C. However there is too much momentum and this pathway becomes unreactive as the collision pushes B back towards A and results in the reformation of the A-B bond.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the collision between A-B and C resulting in the breaking of the A-B bond, followed by the collision of B with C that pushes B back towards C. However in this situation, there is even more momentum so B collides with A and is pushed back towards C, forming a B-C bond and resulting in an overall reactive pathway.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: &lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720921</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720921"/>
		<updated>2018-05-17T17:46:24Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Reactive and Unreactive Trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactivity !! Contour Plot !! Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive || [[File:hys_ex1_traj1.png|400px]] || C approaches A-B and collides. The collision has sufficient momentum for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive || [[File:hys_ex1_traj2.png|400px]] || As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the C moves away from the A-B bond, which remains intact.&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive || [[File:hys_ex1_traj3.png|400px]] || This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive || [[File:hys_ex1_traj4.png|400px]] || This collision has sufficient momentum to break the A-B bond and draw B towards C. However there is too much momentum and this pathway becomes unreactive as the collision pushes B back towards A and results in the reformation of the A-B bond.&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive || [[File:hys_ex1_traj5.png|400px]] || This begins in the same way as the previous situation, with the collision between A-B and C resulting in the breaking of the A-B bond, followed by the collision of B with C that pushes B back towards C. However in this situation, there is even more momentum so B collides with A and is pushed back towards C, forming a B-C bond and resulting in an overall reactive pathway.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: &lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720917</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720917"/>
		<updated>2018-05-17T17:43:44Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Calculating the Reaction Path */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds, as in each time step the velocity is reset to 0, so this provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactive? &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj1.png|400px]] C approaches A-B and collides. The collision has sufficient momentum for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
[[File:hys_ex1_traj2.png|400px]] As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the C moves away from the A-B bond, which remains intact.&lt;br /&gt;
[[File:hys_ex1_traj3.png|400px]]This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj4.png|400px]] This collision has sufficient momentum to break the A-B bond and draw B towards C. However there is too much momentum and this pathway becomes unreactive as the collision pushes B back towards A and results in the reformation of the A-B bond.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj5.png|400px]] This begins in the same way as the previous situation, with the collision between A-B and C resulting in the breaking of the A-B bond, followed by the collision of B with C that pushes B back towards C. However in this situation, there is even more momentum so B collides with A and is pushed back towards C, forming a B-C bond and resulting in an overall reactive pathway.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: &lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720690</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720690"/>
		<updated>2018-05-17T16:40:30Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* F + H2: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds so provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactive? &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj1.png|400px]] C approaches A-B and collides. The collision has sufficient momentum for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
[[File:hys_ex1_traj2.png|400px]] As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the C moves away from the A-B bond, which remains intact.&lt;br /&gt;
[[File:hys_ex1_traj3.png|400px]]This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj4.png|400px]] This collision has sufficient momentum to break the A-B bond and draw B towards C. However there is too much momentum and this pathway becomes unreactive as the collision pushes B back towards A and results in the reformation of the A-B bond.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj5.png|400px]] This begins in the same way as the previous situation, with the collision between A-B and C resulting in the breaking of the A-B bond, followed by the collision of B with C that pushes B back towards C. However in this situation, there is even more momentum so B collides with A and is pushed back towards C, forming a B-C bond and resulting in an overall reactive pathway.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: &lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720689</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720689"/>
		<updated>2018-05-17T16:40:07Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* F-H-H System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds so provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactive? &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj1.png|400px]] C approaches A-B and collides. The collision has sufficient momentum for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
[[File:hys_ex1_traj2.png|400px]] As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the C moves away from the A-B bond, which remains intact.&lt;br /&gt;
[[File:hys_ex1_traj3.png|400px]]This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj4.png|400px]] This collision has sufficient momentum to break the A-B bond and draw B towards C. However there is too much momentum and this pathway becomes unreactive as the collision pushes B back towards A and results in the reformation of the A-B bond.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj5.png|400px]] This begins in the same way as the previous situation, with the collision between A-B and C resulting in the breaking of the A-B bond, followed by the collision of B with C that pushes B back towards C. However in this situation, there is even more momentum so B collides with A and is pushed back towards C, forming a B-C bond and resulting in an overall reactive pathway.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: &lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720687</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720687"/>
		<updated>2018-05-17T16:39:33Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* PES inspection */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds so provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactive? &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj1.png|400px]] C approaches A-B and collides. The collision has sufficient momentum for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
[[File:hys_ex1_traj2.png|400px]] As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the C moves away from the A-B bond, which remains intact.&lt;br /&gt;
[[File:hys_ex1_traj3.png|400px]]This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj4.png|400px]] This collision has sufficient momentum to break the A-B bond and draw B towards C. However there is too much momentum and this pathway becomes unreactive as the collision pushes B back towards A and results in the reformation of the A-B bond.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj5.png|400px]] This begins in the same way as the previous situation, with the collision between A-B and C resulting in the breaking of the A-B bond, followed by the collision of B with C that pushes B back towards C. However in this situation, there is even more momentum so B collides with A and is pushed back towards C, forming a B-C bond and resulting in an overall reactive pathway.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: [[File:hys_ex2_FHpes.png|400px]]&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below: [[File:hys_ex2_FHpes2.png|400px]]&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png|400px]]&lt;br /&gt;
[[File:hys_ex2_tsdvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720683</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720683"/>
		<updated>2018-05-17T16:39:03Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds so provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactive? &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj1.png|400px]] C approaches A-B and collides. The collision has sufficient momentum for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
[[File:hys_ex1_traj2.png|400px]] As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the C moves away from the A-B bond, which remains intact.&lt;br /&gt;
[[File:hys_ex1_traj3.png|400px]]This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj4.png|400px]] This collision has sufficient momentum to break the A-B bond and draw B towards C. However there is too much momentum and this pathway becomes unreactive as the collision pushes B back towards A and results in the reformation of the A-B bond.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj5.png|400px]] This begins in the same way as the previous situation, with the collision between A-B and C resulting in the breaking of the A-B bond, followed by the collision of B with C that pushes B back towards C. However in this situation, there is even more momentum so B collides with A and is pushed back towards C, forming a B-C bond and resulting in an overall reactive pathway.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: [[File:hys_ex2_FHpes.png]]&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below: [[File:hys_ex2_FHpes2.png]]&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png]]&lt;br /&gt;
[[File:hys_ex2_tsdvt.png]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png|400px]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720681</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720681"/>
		<updated>2018-05-17T16:38:37Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds so provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactive? &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj1.png|400px]] C approaches A-B and collides. The collision has sufficient momentum for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
[[File:hys_ex1_traj2.png|400px]] As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the C moves away from the A-B bond, which remains intact.&lt;br /&gt;
[[File:hys_ex1_traj3.png|400px]]This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj4.png|400px]] This collision has sufficient momentum to break the A-B bond and draw B towards C. However there is too much momentum and this pathway becomes unreactive as the collision pushes B back towards A and results in the reformation of the A-B bond.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj5.png|400px]] This begins in the same way as the previous situation, with the collision between A-B and C resulting in the breaking of the A-B bond, followed by the collision of B with C that pushes B back towards C. However in this situation, there is even more momentum so B collides with A and is pushed back towards C, forming a B-C bond and resulting in an overall reactive pathway.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: [[File:hys_ex2_FHpes.png]]&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below: [[File:hys_ex2_FHpes2.png]]&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png]]&lt;br /&gt;
[[File:hys_ex2_tsdvt.png]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
====Reaction Energy====&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_cont_new.png&amp;diff=720666</id>
		<title>File:Hys ex2 dyn cont new.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_cont_new.png&amp;diff=720666"/>
		<updated>2018-05-17T16:35:38Z</updated>

		<summary type="html">&lt;p&gt;Hys116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720664</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720664"/>
		<updated>2018-05-17T16:35:19Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* F + H2: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds so provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactive? &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj1.png|400px]] C approaches A-B and collides. The collision has sufficient momentum for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
[[File:hys_ex1_traj2.png|400px]] As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the C moves away from the A-B bond, which remains intact.&lt;br /&gt;
[[File:hys_ex1_traj3.png|400px]]This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj4.png|400px]] This collision has sufficient momentum to break the A-B bond and draw B towards C. However there is too much momentum and this pathway becomes unreactive as the collision pushes B back towards A and results in the reformation of the A-B bond.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj5.png|400px]] This begins in the same way as the previous situation, with the collision between A-B and C resulting in the breaking of the A-B bond, followed by the collision of B with C that pushes B back towards C. However in this situation, there is even more momentum so B collides with A and is pushed back towards C, forming a B-C bond and resulting in an overall reactive pathway.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: [[File:hys_ex2_FHpes.png]]&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below: [[File:hys_ex2_FHpes2.png]]&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png]]&lt;br /&gt;
[[File:hys_ex2_tsdvt.png]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_cont3.png&amp;diff=720661</id>
		<title>File:Hys ex2 dyn cont3.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_cont3.png&amp;diff=720661"/>
		<updated>2018-05-17T16:35:00Z</updated>

		<summary type="html">&lt;p&gt;Hys116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_cont-3.png&amp;diff=720656</id>
		<title>File:Hys ex2 dyn cont-3.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_cont-3.png&amp;diff=720656"/>
		<updated>2018-05-17T16:34:39Z</updated>

		<summary type="html">&lt;p&gt;Hys116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_cont0.png&amp;diff=720653</id>
		<title>File:Hys ex2 dyn cont0.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_cont0.png&amp;diff=720653"/>
		<updated>2018-05-17T16:34:09Z</updated>

		<summary type="html">&lt;p&gt;Hys116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn2_works.png&amp;diff=720651</id>
		<title>File:Hys ex2 dyn2 works.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn2_works.png&amp;diff=720651"/>
		<updated>2018-05-17T16:33:47Z</updated>

		<summary type="html">&lt;p&gt;Hys116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720647</id>
		<title>MRD:hys116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:hys116&amp;diff=720647"/>
		<updated>2018-05-17T16:33:28Z</updated>

		<summary type="html">&lt;p&gt;Hys116: /* HF + H */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System==&lt;br /&gt;
===Transition State===&lt;br /&gt;
At both the minima and at the transition state, the gradient of the potential energy surface is 0. This is a saddle point with both the maxima of the transition state and the minima in the same position but they can be identified using their second derivative and the shape of the curvature of the plot. The second derivative of the transition state is less than 0 as it is a maximum and this can be identified from the potential energy curve as the curve between the base of the plot and the minimum energy path. The second derivative of the minima is greater than 0 and is the minimum point in the minimum energy path.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_PES.png|500px]]&lt;br /&gt;
&lt;br /&gt;
The transition state position has been estimated to be 0.9076. From the contour plot, this is where the atoms are in the same position, not falling off the ridge and there is no orthognoal gradient acting on the system. &lt;br /&gt;
From the plot of internuclear distance vs time, this position shows no oscillation as there is no momentum in the system so the transition state is still. The internuclear distance of A-B is equal to B-C and this is seen in the plot of internuclear distance vs time in which the corresponding two lines are overlapping.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_contour.png|400px]][[File:hys_ex1_intvt.png|400px]]&lt;br /&gt;
&lt;br /&gt;
===Calculating the Reaction Path===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_mep.png|400px]][[File:hys_ex1_trajectory.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The MEP diagram  shows a straight line for the trajectory whereas the dynamic trajectory is a wavy line. This is because it does not take into account oscillations of the bonds so provides a slightly less accurate path.&lt;br /&gt;
&lt;br /&gt;
===Internuclear distance and momenta at large t===&lt;br /&gt;
&lt;br /&gt;
Double check these graphs??&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_dvt.png|300px]][[File:hys_ex1_mvt.png|300px]]&lt;br /&gt;
&lt;br /&gt;
As time increases, A-B bond distance increases whereas B-C bond distance roughly constant; atoms B and C stay relatively stationary while atom A moves away. &lt;br /&gt;
&lt;br /&gt;
With reversed thing:&lt;br /&gt;
[[File:hys_ex1_dvtrev.png|300px]][[File:hys_ex1_mvtrev.png|300px]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy !! Reactive? &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || -100.456 || Unreactive &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || -98.956 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || -84.956 || Uneactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || -83.416 || Reactive&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj1.png|400px]] C approaches A-B and collides. The collision has sufficient momentum for a reaction to occur. The A-B bond breaks and a B-C bond is formed and the molecules move in opposite directions.&lt;br /&gt;
[[File:hys_ex1_traj2.png|400px]] As before, C approaches A-B and collides. However, the collision does not have enough momentum for a reaction to occur so the C moves away from the A-B bond, which remains intact.&lt;br /&gt;
[[File:hys_ex1_traj3.png|400px]]This is very similar to the first situation as there is sufficient momentum for the collision to result in a reaction and the A-B bond to break. A-B has a slightly lower momentum than in the first situation so it takes slightly longer for the reaction to occur.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj4.png|400px]] This collision has sufficient momentum to break the A-B bond and draw B towards C. However there is too much momentum and this pathway becomes unreactive as the collision pushes B back towards A and results in the reformation of the A-B bond.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex1_traj5.png|400px]] This begins in the same way as the previous situation, with the collision between A-B and C resulting in the breaking of the A-B bond, followed by the collision of B with C that pushes B back towards C. However in this situation, there is even more momentum so B collides with A and is pushed back towards C, forming a B-C bond and resulting in an overall reactive pathway.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
Transitions State Theory is used to predict reaction rates and is based on a number of assumptions. It assumes that nuclei behave classically, and ignores the effect of quantum tunnelling. According to classical mechanics, a collision between reacting atoms/molecules must have energy greater than or equal to the activation energy in order for the reaction to occur. However, quantum tunnelling allows particles to tunnel through energy barriers that they cannot get over classically, meaning molecules can react, even if their collisions do not have energy ≥ E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;.  Tunnelling is more likely in reactions with low activation energy.&lt;br /&gt;
&lt;br /&gt;
Another assumption is that intermediates formed are long-lived, however this does not affect the results in this experiment as this is an elementary reaction with no intermediates. It is also assumed that the reaction trajectory is acrsoss the lowest energy saddle point, however at high temperatures molecules can be in higher vibrational energy levels so different, higher energy transition states may exist.&lt;br /&gt;
&lt;br /&gt;
The experimental values obtained are likely to be similar to the Transition State Theory predictions however there will be small systematic differences due to quantum tunnelling and molecules in higher vibrational modes, which can be reduced by carrying out calculations at low temperatures.&lt;br /&gt;
&lt;br /&gt;
==F-H-H System==&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; HF + H ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
F H distance: 2.30&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
F H momentum: -2.7&lt;br /&gt;
H-H momentum: 0&lt;br /&gt;
This produced the surface plot shown below: [[File:hys_ex2_FHpes.png]]&lt;br /&gt;
The reaction is exothermic as the products are lower in energy than the reactants. This suggests that the H-F bond formed is stronger than the H-H bond broken.&lt;br /&gt;
&lt;br /&gt;
====H + HF ---&amp;gt; + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F ====&lt;br /&gt;
Using the inital conditions:&lt;br /&gt;
H H distance: 2.30&lt;br /&gt;
H-F distance: 0.74&lt;br /&gt;
H H momentum: -5&lt;br /&gt;
H-F momentum: 0&lt;br /&gt;
This produced the surface plot shown below: [[File:hys_ex2_FHpes2.png]]&lt;br /&gt;
The reaction is endothermic as the products are higher in energy than the reactants. Again, this suggests that the H-F bond broken is stronger than the H-H bond formed.&lt;br /&gt;
&lt;br /&gt;
====Transition State====&lt;br /&gt;
Transition state distances were estimated to be:&lt;br /&gt;
H-H bond distance = 0.7465&lt;br /&gt;
H-F bond distance = 1.8095&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_tscont.png]]&lt;br /&gt;
[[File:hys_ex2_tsdvt.png]]&lt;br /&gt;
&lt;br /&gt;
At these distances, the contour plot shows no reaction trajectory and the plot of internuclear distances vs time shows minimum oscillation.&lt;br /&gt;
&lt;br /&gt;
====Activation Energies====&lt;br /&gt;
Energy of the transition state: -103.751 kcal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepts.png]]&lt;br /&gt;
&lt;br /&gt;
Energy of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: -103.761 (moved 2.3)&lt;br /&gt;
&lt;br /&gt;
Energy of H + HF: -133.880 (Using 0.92 as HF bond length and H H distance as 2.3)&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
Set H-F length to ts - 0.1 then use last geometries to find energies:&lt;br /&gt;
Energy of H + HF: -133.762&lt;br /&gt;
Set H-F length to ts+0.1 then use last geometries:&lt;br /&gt;
Energy of F + H2: -103.752&lt;br /&gt;
&lt;br /&gt;
Transitions state of 1:&lt;br /&gt;
Transition state of 2:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r1.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mepwe.png]]&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_mep_r2.png]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics===&lt;br /&gt;
The following conditions were found to result in a reactive trajectory shown in the contour plot below:&lt;br /&gt;
H F distance: 2.3&lt;br /&gt;
H-H distance: 0.74&lt;br /&gt;
H F momenutm: -2&lt;br /&gt;
H-H momentum: 2.7&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_cont.png]]&lt;br /&gt;
&lt;br /&gt;
The H2 molecule approaches F and collides. H-H bond breaks and one H atom collides with F, bounces back and collides with other H then bounces back to form H-F bond.&lt;br /&gt;
&lt;br /&gt;
Momentum vs time graph is shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_mvt.png]]&lt;br /&gt;
&lt;br /&gt;
Before the collision, this graph shows that H2 (BC) has kinetic energy in shown by the oscillations in the graph. After the collision, the line for H2 shows no oscillation; this energy has been converted into potential energy. F-H (AB) shows the opposite pattern. Energy is conserved, so on collision, the kinetic energy of H2 is transferred to HF. This is supported by the energy v time graph shown below:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn_evt.png]]&lt;br /&gt;
&lt;br /&gt;
This could be determined experimentally by looking at the IR spectra of the reactants and the products as the energy of the oscillations of the bonds is conserved during the reaction.&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules ====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s empirical rules state that for reactions with late transition states, such as the endothermic reaction of HF + H, vibrational energy has a larger effect on the efficiency of the reaction than translational energy.&lt;br /&gt;
For reactions with early transition states, such as the exothermic reaction of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, translational energy has a larger effect than vibrational energy.&lt;br /&gt;
&lt;br /&gt;
===== HF + H=====&lt;br /&gt;
This reaction is endothermic so has a late transition state. Therefore increasing the vibrational energy of HF and decreasing the translational energy of the incoming H increases the efficiency of the reaction as shown below&lt;br /&gt;
Initial conditions:&lt;br /&gt;
H-F distance: 0.91&lt;br /&gt;
H H distance: 2.3&lt;br /&gt;
The momentum of the incoming H atom was started at -2.5 and the HF momentum at 0.1.&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_no.png|400px]]&lt;br /&gt;
&lt;br /&gt;
When p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; (vibrational energy) is increased to 1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; (translational energy) is decreased to -10, a reactive trajectory is found:&lt;br /&gt;
&lt;br /&gt;
[[File:hys_ex2_dyn2_works.png|400px]]&lt;br /&gt;
&lt;br /&gt;
=====F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;:=====&lt;br /&gt;
This reaction is exothermic so has an early transition state. Therefore increasing the translational energy of F and decreasing the vibrational energy of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; increases the efficiency of the reaction.&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy is varied between -3 and 3, this effect can be seen. When the vibrational energy (HH momentum) is close to 0, the reaction is successful?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F H distance: 2&lt;br /&gt;
H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: 0.74&lt;br /&gt;
F H momentum: -0.5&lt;br /&gt;
&lt;br /&gt;
When the vibrational energy (HH momentum) is close to 0, the reaction is successful:&lt;br /&gt;
[[File:hys_ex2_dyn_cont0.png|400px]]&lt;br /&gt;
&lt;br /&gt;
As vibrational energy increases (further away from 0), the reaction becomes unsuccessful:&lt;br /&gt;
[[File:hys_ex2_dyn_cont-3.png|400px]]&lt;br /&gt;
[[File:hys_ex2_dyn_cont3.png|400px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For same positions but:&lt;br /&gt;
&lt;br /&gt;
F H momentum: -0.8&lt;br /&gt;
H-H momentum: 0.1&lt;br /&gt;
[[File:hys_ex2_dyn_cont_new.png|400px]]&lt;br /&gt;
This is reactive. In this example, the translational motion of F has been increased and the vibrational energy has been decreased. From Polanyi&#039;s rules, this increases the efficiency of the reaction, as supported by the contour plot above.&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn2_no.png&amp;diff=720641</id>
		<title>File:Hys ex2 dyn2 no.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn2_no.png&amp;diff=720641"/>
		<updated>2018-05-17T16:32:49Z</updated>

		<summary type="html">&lt;p&gt;Hys116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_evt.png&amp;diff=720638</id>
		<title>File:Hys ex2 dyn evt.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_evt.png&amp;diff=720638"/>
		<updated>2018-05-17T16:32:22Z</updated>

		<summary type="html">&lt;p&gt;Hys116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_mvt.png&amp;diff=720636</id>
		<title>File:Hys ex2 dyn mvt.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_mvt.png&amp;diff=720636"/>
		<updated>2018-05-17T16:31:59Z</updated>

		<summary type="html">&lt;p&gt;Hys116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_cont.png&amp;diff=720632</id>
		<title>File:Hys ex2 dyn cont.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hys_ex2_dyn_cont.png&amp;diff=720632"/>
		<updated>2018-05-17T16:31:28Z</updated>

		<summary type="html">&lt;p&gt;Hys116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hys116</name></author>
	</entry>
</feed>