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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804868</id>
		<title>MRD:01533249</title>
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		<updated>2020-05-15T16:36:35Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot.&amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt; It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the geometry of the transition state was made, where each component had zero momentum, it would remain at that point and not roll down to the reactant or product valley.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefore they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry of contour plot system is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy as it has a stringer bond. The strength of the bond is due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of the lines is zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. &amp;lt;ref name=&amp;quot;BombCal&amp;quot;/&amp;gt; However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity.&amp;lt;ref name=&amp;quot;Chemi&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by early release of the reaction energy in the reactants valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Chemi&amp;quot;&amp;gt;Karabulut, E. and Sidir, İ., 2018. The analysis of HF molecule by means of infrared transitions in H + F2 collinear scattering on two different potential energy surfaces. Chemical Physics Letters, 709, pp.103-109.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
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		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804865"/>
		<updated>2020-05-15T16:36:14Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot.&amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt; It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the geometry of the transition state was made, where each component had zero momentum, it would remain at that point and not roll down to the reactant or product valley.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefore they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry of contour plot system is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy as it has a stringer bond. The strength of the bond is due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of the lines is zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. &amp;lt;ref name=&amp;quot;BombCal&amp;quot;/&amp;gt; However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity.&amp;lt;ref name=&amp;quot;Chemi&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by early release of the reaction energy in the reactants valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Chemi&amp;quot;&amp;gt;Karabulut, E. and Sidir, İ., 2018. The analysis of HF molecule by means of infrared transitions in H + F2 collinear scattering on two different potential energy surfaces. Chemical Physics Letters, 709, pp.103-109.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804831</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804831"/>
		<updated>2020-05-15T16:29:22Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* PES inspection */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot.&amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt; It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the geometry of the transition state was made, where each component had zero momentum, it would remain at that point and not roll down to the reactant or product valley.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefore they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry of contour plot system is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy as it has a stringer bond. The strength of the bond is due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of the lines is zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. &amp;lt;ref name=&amp;quot;BombCal&amp;quot;/&amp;gt; However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity.&amp;lt;ref name=&amp;quot;Chemi&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Chemi&amp;quot;&amp;gt;Karabulut, E. and Sidir, İ., 2018. The analysis of HF molecule by means of infrared transitions in H + F2 collinear scattering on two different potential energy surfaces. Chemical Physics Letters, 709, pp.103-109.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804828</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804828"/>
		<updated>2020-05-15T16:28:17Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* PES inspection */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot.&amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt; It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the geometry of the transition state was made, where each component had zero momentum, it would remain at that point and not roll down to the reactant or product valley.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefore they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry of contour plot system is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy as it has a stringer bond. The strength of the bond is due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. &amp;lt;ref name=&amp;quot;BombCal&amp;quot;/&amp;gt; However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity.&amp;lt;ref name=&amp;quot;Chemi&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Chemi&amp;quot;&amp;gt;Karabulut, E. and Sidir, İ., 2018. The analysis of HF molecule by means of infrared transitions in H + F2 collinear scattering on two different potential energy surfaces. Chemical Physics Letters, 709, pp.103-109.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804821</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804821"/>
		<updated>2020-05-15T16:22:33Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* MEP and Dynamic Trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot.&amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt; It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the geometry of the transition state was made, where each component had zero momentum, it would remain at that point and not roll down to the reactant or product valley.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefore they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry of contour plot system is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. &amp;lt;ref name=&amp;quot;BombCal&amp;quot;/&amp;gt; However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity.&amp;lt;ref name=&amp;quot;Chemi&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Chemi&amp;quot;&amp;gt;Karabulut, E. and Sidir, İ., 2018. The analysis of HF molecule by means of infrared transitions in H + F2 collinear scattering on two different potential energy surfaces. Chemical Physics Letters, 709, pp.103-109.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804817</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804817"/>
		<updated>2020-05-15T16:20:46Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* MEP and Dynamic Trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot.&amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt; It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the geometry of the transition state was made, where each component had zero momentum, it would remain at that point and not roll down to the reactant or product valley.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefore they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. &amp;lt;ref name=&amp;quot;BombCal&amp;quot;/&amp;gt; However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity.&amp;lt;ref name=&amp;quot;Chemi&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Chemi&amp;quot;&amp;gt;Karabulut, E. and Sidir, İ., 2018. The analysis of HF molecule by means of infrared transitions in H + F2 collinear scattering on two different potential energy surfaces. Chemical Physics Letters, 709, pp.103-109.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804813</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804813"/>
		<updated>2020-05-15T16:19:05Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Transition State */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot.&amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt; It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the geometry of the transition state was made, where each component had zero momentum, it would remain at that point and not roll down to the reactant or product valley.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. &amp;lt;ref name=&amp;quot;BombCal&amp;quot;/&amp;gt; However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity.&amp;lt;ref name=&amp;quot;Chemi&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Chemi&amp;quot;&amp;gt;Karabulut, E. and Sidir, İ., 2018. The analysis of HF molecule by means of infrared transitions in H + F2 collinear scattering on two different potential energy surfaces. Chemical Physics Letters, 709, pp.103-109.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804811</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804811"/>
		<updated>2020-05-15T16:17:25Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Transition State */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot.&amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt; It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. &amp;lt;ref name=&amp;quot;BombCal&amp;quot;/&amp;gt; However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity.&amp;lt;ref name=&amp;quot;Chemi&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Chemi&amp;quot;&amp;gt;Karabulut, E. and Sidir, İ., 2018. The analysis of HF molecule by means of infrared transitions in H + F2 collinear scattering on two different potential energy surfaces. Chemical Physics Letters, 709, pp.103-109.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804810</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804810"/>
		<updated>2020-05-15T16:16:53Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. &amp;lt;ref name=&amp;quot;BombCal&amp;quot;/&amp;gt; However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity.&amp;lt;ref name=&amp;quot;Chemi&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Chemi&amp;quot;&amp;gt;Karabulut, E. and Sidir, İ., 2018. The analysis of HF molecule by means of infrared transitions in H + F2 collinear scattering on two different potential energy surfaces. Chemical Physics Letters, 709, pp.103-109.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804775</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804775"/>
		<updated>2020-05-15T15:57:36Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. &amp;lt;ref name=&amp;quot;BombCal&amp;quot;/&amp;gt; However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity.&amp;lt;ref name=&amp;quot;Chemi&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Chemi&amp;quot;&amp;gt;Karabulut, E. and Sidir, İ., 2018. The analysis of HF molecule by means of infrared transitions in H + F2 collinear scattering on two different potential energy surfaces. Chemical Physics Letters, 709, pp.103-109.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804773</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804773"/>
		<updated>2020-05-15T15:57:09Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. &amp;lt;ref name=&amp;quot;BombCal&amp;quot;/&amp;gt; However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity.&amp;lt;ref name=&amp;quot;Chemi&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804762</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804762"/>
		<updated>2020-05-15T15:49:11Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. &amp;lt;ref name=&amp;quot;BombCal&amp;quot;/&amp;gt; However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804760</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804760"/>
		<updated>2020-05-15T15:48:40Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;BombCal&amp;quot;&amp;gt;Atkins, P. and De Paula, J., 2014. Atkins&#039; Physical Chemistry. 10th ed. Oxford: Oxford University Press, p.71.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804752</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804752"/>
		<updated>2020-05-15T15:41:30Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;TST&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.49.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804749</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804749"/>
		<updated>2020-05-15T15:40:38Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Transition State Theory */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants.&amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not. Another assumption is transition state  theory is a classical theory &amp;lt;ref name=&amp;quot;TST&amp;quot;/&amp;gt; and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804744</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804744"/>
		<updated>2020-05-15T15:36:59Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants. This can be joined with Hammonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804743</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804743"/>
		<updated>2020-05-15T15:36:34Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
Polanyi&#039;s rule states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products.&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;/&amp;gt; &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804741</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804741"/>
		<updated>2020-05-15T15:35:41Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;HammondsPostulant&amp;quot;&amp;gt;Scala, A., 2004. Free Radical Halogenation, Selectivity, and Thermodynamics: The Polanyi Principle and Hammond&#039;s Postulate. Journal of Chemical Education, 81(11), p.1661.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804738</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804738"/>
		<updated>2020-05-15T15:31:55Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804737</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804737"/>
		<updated>2020-05-15T15:31:44Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;PolanyiRule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Polanyi&#039;s rule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804736</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804736"/>
		<updated>2020-05-15T15:30:36Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;Polanyi.27s_Rule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Polanyi&#039;s rule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804734</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804734"/>
		<updated>2020-05-15T15:29:52Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface.&amp;lt;ref name=&amp;quot;Polanyi&#039;s Rule&amp;quot; /&amp;gt;&lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;Polanyi&#039;s rule&amp;quot;&amp;gt;Brouard, M., 1998. Reaction Dynamics. [S.l.]: Oxford University Press, p.37..&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804720</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804720"/>
		<updated>2020-05-15T15:13:11Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|-&lt;br /&gt;
| -1&lt;br /&gt;
| -12&lt;br /&gt;
|[[File:Contour-hfh-1-12-01533249.png|300px]]&lt;br /&gt;
| This is unreactive. The reaction doesn&#039;t occur this is because the reactant has a very low vibrational energy. Vibrational Energy in the reactants promotes endothermic reactions due to their late transition states. &lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour-hfh-1-12-01533249.png&amp;diff=804708</id>
		<title>File:Contour-hfh-1-12-01533249.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour-hfh-1-12-01533249.png&amp;diff=804708"/>
		<updated>2020-05-15T15:08:25Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804687</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804687"/>
		<updated>2020-05-15T15:05:49Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804685</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804685"/>
		<updated>2020-05-15T15:05:31Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
===Reactive and unreactive trajectories===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804683</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804683"/>
		<updated>2020-05-15T15:05:02Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Exercise 2: F-H-H system */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
===PES inspection ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
=Reactive and unreactive trajectories=&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804681</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804681"/>
		<updated>2020-05-15T15:03:59Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
The amount if energy released can be calculated experimentally using &#039;Bomb Calorimetry&#039;, this tests for a change in temperature produced by the release in energy. However this experiment cannot distinguish between the translational and vibrational energy produced. The vibrational energy can be monitored experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
=Reactive and unreactive trajectories=&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804659</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804659"/>
		<updated>2020-05-15T14:54:54Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
This can be tested experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore the reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804656</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804656"/>
		<updated>2020-05-15T14:54:11Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
This can be tested experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore they reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 74 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 200 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804653</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804653"/>
		<updated>2020-05-15T14:53:12Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
This can be tested experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Reactive trajectory.&lt;br /&gt;
At the geometry  r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm, and the momentums p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. There is a reactive trajectory (figure 4). H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F is an exothermic reaction and hence is promoted by a large translational excitation of the products this can be clearly seen in this case, even though there is   a very small vibrational excitation of the products.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore they reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File:Contour-hfh-9-3-0153349.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions. Although the reaction passes the transition state more than once the products are eventually formed.&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804649</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804649"/>
		<updated>2020-05-15T14:51:02Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
This can be tested experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Reactive trajectory.&lt;br /&gt;
At the geometry  r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm, and the momentums p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. There is a reactive trajectory (figure 4). H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F is an exothermic reaction and hence is promoted by a large translational excitation of the products this can be clearly seen in this case, even though there is   a very small vibrational excitation of the products.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore they reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;HF + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -9&lt;br /&gt;
| -3&lt;br /&gt;
|[[File: Contour-hfh-9-3-01533249.png|300px]]&lt;br /&gt;
| The reaction is endothermic, in this case there is a large vibrational energy of the reactants, the fact that the reaction has occurred follows Polanyi&#039;s rules as the vibration energy of the reactants promotes endothermic reactions.&lt;br /&gt;
&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour-hfh-9-3-0153349.png&amp;diff=804636</id>
		<title>File:Contour-hfh-9-3-0153349.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour-hfh-9-3-0153349.png&amp;diff=804636"/>
		<updated>2020-05-15T14:46:06Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804549</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804549"/>
		<updated>2020-05-15T14:27:06Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
This can be tested experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Reactive trajectory.&lt;br /&gt;
At the geometry  r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm, and the momentums p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. There is a reactive trajectory (figure 4). H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F is an exothermic reaction and hence is promoted by a large translational excitation of the products this can be clearly seen in this case, even though there is   a very small vibrational excitation of the products.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefore favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore they reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
| In this case the reactants have enough energy to form the products with a large amount of translational energy which is then released into the products, which I favoured in exothermic reactions as shown in Polanyi&#039;s rules shown above.&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804520</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804520"/>
		<updated>2020-05-15T14:17:28Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
This can be tested experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Reactive trajectory.&lt;br /&gt;
At the geometry  r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm, and the momentums p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. There is a reactive trajectory (figure 4). H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F is an exothermic reaction and hence is promoted by a large translational excitation of the products this can be clearly seen in this case, even though there is   a very small vibrational excitation of the products.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot||&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6-01533249.png|300px]]&lt;br /&gt;
| The reaction is exothermic and is therefor favoured by the translational energy of the products, in this case the reactants have enough energy to reach the transition state and form the products however these products don&#039;t have enough translational energy to escape and therefore they reactants are reformed.&lt;br /&gt;
|-&lt;br /&gt;
| -1.0&lt;br /&gt;
| 6&lt;br /&gt;
|[[File:Contour-1-6-01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour-1-6-01533249.png&amp;diff=804516</id>
		<title>File:Contour-1-6-01533249.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour-1-6-01533249.png&amp;diff=804516"/>
		<updated>2020-05-15T14:16:14Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804484</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804484"/>
		<updated>2020-05-15T14:10:40Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
This can be tested experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Reactive trajectory.&lt;br /&gt;
At the geometry  r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm, and the momentums p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. There is a reactive trajectory (figure 4). H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F is an exothermic reaction and hence is promoted by a large translational excitation of the products this can be clearly seen in this case, even though there is   a very small vibrational excitation of the products.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|  p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup.|| p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup||Contour Plot&lt;br /&gt;
|-&lt;br /&gt;
| -1.6&lt;br /&gt;
| 0.2&lt;br /&gt;
|[[File: Contour-hf-1_6_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour-hf-1_6-01533249.png&amp;diff=804467</id>
		<title>File:Contour-hf-1 6-01533249.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour-hf-1_6-01533249.png&amp;diff=804467"/>
		<updated>2020-05-15T14:05:10Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804434</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=804434"/>
		<updated>2020-05-15T13:50:38Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
This can be tested experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H2 + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Reactive trajectory.&lt;br /&gt;
At the geometry  r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 200 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74 pm, and the momentums p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. There is a reactive trajectory (figure 4). H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + F is an exothermic reaction and hence is promoted by a large translational excitation of the products this can be clearly seen in this case, even though there is   a very small vibrational excitation of the products.&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803976</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803976"/>
		<updated>2020-05-15T10:26:36Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
This can be tested experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by vibrational excitation of the reactants.&lt;br /&gt;
This can be joined with Hamonds postulant, that exothermic reactions the transition state is closer to the reactants and in endothermic reactions the transition state is closer to the products. &lt;br /&gt;
&lt;br /&gt;
Together we can tell that in order to promote exothermic reactions translation excitation of the products will promote the reaction. In order to promote endothermic reactions vibrational excitation of the reactants should promote this reaction.&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803452</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803452"/>
		<updated>2020-05-14T18:45:23Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
This can be tested experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by translational excitation of the products. Reactions with the transition state closer to the products will be promoted best by excitation of the reactants.&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803406</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803406"/>
		<updated>2020-05-14T18:06:57Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
This can be tested experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Polanyi&#039;s rule&#039;&#039;&#039; states that the vibrational excitation in the products is enhanced by the increasing early release of the reaction energy in the entrance valley of the potential energy surface. &lt;br /&gt;
It therefore suggests that the reactions with a transition state closer to the reactants will be promoted by initial translational excitation and products with the transition state closer to the products will be promoted best by excitation of the reactants&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803356</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803356"/>
		<updated>2020-05-14T17:29:06Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;br /&gt;
&lt;br /&gt;
This can be tested experimentally using chemiluminescence where the rotational and vibrational population distribution can be seen by analyse of Infrared chemiluminescence intensity. &#039;&#039;&#039;https://pubs.acs.org/doi/pdf/10.1021/j100524a018&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803338</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803338"/>
		<updated>2020-05-14T17:03:16Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;br /&gt;
&lt;br /&gt;
[[File:Momentum-hf-rd-01533249.png|400px|thumb|none|Momentum vs Time plot showing the conservation of energy.]]&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Momentum-hf-rd-01533249.png&amp;diff=803337</id>
		<title>File:Momentum-hf-rd-01533249.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Momentum-hf-rd-01533249.png&amp;diff=803337"/>
		<updated>2020-05-14T17:01:26Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803333</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803333"/>
		<updated>2020-05-14T16:56:19Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Exercise 2: F-H-H system */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state.&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. The positions are  n this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; the values is taken from figure 2 below. The positions in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 90 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 165 pm. This is small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state for HF + H system.]]&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy_ae_exo_01533249.png|400px|thumb|none| Figure 2: Energy vs Time plot offset the transition state for H2 + F system.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Energy_ae_exo_01533249.png&amp;diff=803328</id>
		<title>File:Energy ae exo 01533249.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Energy_ae_exo_01533249.png&amp;diff=803328"/>
		<updated>2020-05-14T16:53:19Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803312</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803312"/>
		<updated>2020-05-14T16:48:06Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Exercise 2: F-H-H system */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state: in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H+HF&#039;&#039;&#039; reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below. This is a large activation energy as the reaction is endothermic and energy is required to reach the transition state. The transition state is closer in structure to the products in this case&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the &#039;&#039;&#039;H2 + F&#039;&#039;&#039; reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; . This is  small activation energy as the reaction is exothermic and little energy is required to make the reaction start. The transition state is close in structure to the reactants in this case.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039; = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;/div&gt;</summary>
		<author><name>Lec4918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803292</id>
		<title>MRD:01533249</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01533249&amp;diff=803292"/>
		<updated>2020-05-14T16:36:21Z</updated>

		<summary type="html">&lt;p&gt;Lec4918: /* Exercise 2: F-H-H system */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Excersise 1 H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===Transition State===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The transition state is the saddle point on the potential energy surface plot. It is the maximum energy point on the reaction pathway but on the path orthogonal to the reaction pathway it is a minimum. It is mathematically defined as the point at which dV/dr = 0, (the gradient is zero), with a negative second derivative in direction of the reaction pathway an positive second derivative orthogonal in direction to the reaction pathway. It can be therefor distinguished from local minima by looking at the second derivatives. If the position of the transition state was made with no momentum it would remain at that given position.&lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot_energy_maximum.png|400px|thumb|none|The transition point is the maximum on the reaction pathway]]&lt;br /&gt;
[[File:Surface_Plot_energy_minimum.png|400px|thumb|none|The transition point is the minimum point.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this set up, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; the system is symmetrical and therefore the distance between the atoms at the transition state is the same for both atoms r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The transition state can be found by looking for the point at which the forces along both the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bonds is = 0 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. On a surface plot, it the energy maximum on the minimum energy path of the reaction. [[File:Surface_Plot_H2_ts_01533249.png|300px|thumb|none|A Surface Plot: the Transition state is the black dot.]]&lt;br /&gt;
&lt;br /&gt;
It can also be identified as the positions at which there is no change in distance over time. The Internuclear Distances vs Time plots would therefore have 2 straight lines each with a gradient of zero. [[File:dist_vs_time_H2_TS_01533249.png|300px|thumb|none|A Internuclear Distances vs Time graph of the Transition state.]]&lt;br /&gt;
&lt;br /&gt;
The transition state position was found by the trial and error technique, changing the r values  between a range of 80 and 100 pm, whilst r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; and the momentum of each molecule was 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. rts was found to be 90.777 pm. The range of r values to test was chosen by visualising approximately where the rts was on a contour plot,&lt;br /&gt;
[[File:Contour_Plot_H2_TS_01533249.png|300px|thumb|none|A Contour Plot  of the with the transition state marked in red.]]&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Trajectories ===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
With the new initial conditions the system is displaced from the transition state with r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=rts + 1 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= rts. This means that the length of the r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is now longer hence the transition state was overcome and the reaction &#039;rolls&#039;  to the products, as the length of the r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; increases, as seen in the contour plot. The MEP calculation contour plot shows the increase of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; in a straight line, opposed to the dynamic calculation contour plot which shows it as an oscillating line. The oscillating line is the vibrations of the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond due to the release of energy as the bond forms. The fact that the  MEP calculation doesn&#039;t see the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond as vibrating, suggests the energy released from the formation of the bond is not conserved. This can also be viewed clearly in the Distances vs Time plots, in the MEP plot the B-C (orange) line is flat whereas in the Dynamic plot the B-C (orange) line is oscillating.&lt;br /&gt;
&lt;br /&gt;
The trajectories can also be looked at through a Momentum vs Time plot; although the initial conditions start with no momentum, they are just off set of the transition state, an energy maximum, and their end trajectory is the energy minimum (the products in this case) therefor they start with a degree of potential energy and this must be lost and turned into kinetic energy (momentum). This is followed in the dynamic calculations plot however the MEP calculations plot do not conserve energy hence there is a no change in momentum observed. &lt;br /&gt;
If the final geometry is used with the momentum signs reversed on a dynamic calculation the trajectory ends back at the starting position just offset of the rts. However if this same calculation is done in MEP calculation the trajectory continues in the same direction.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ &#039;&#039;&#039;MEP and Dynamic plots&#039;&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
| ||MEP||Dynamic&lt;br /&gt;
|-&lt;br /&gt;
|Contour&lt;br /&gt;
|[[File:contour_plot_h2_mep_01533249.png|300px]] &lt;br /&gt;
|[[File: contour_h2_dyn_01533249.png|300px]]&lt;br /&gt;
 |-&lt;br /&gt;
|Distance vs Time&lt;br /&gt;
|[[File:dist_vs_time_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[File:dist_vs_time_h2_dyn_01533249.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
|Momentum vs Time&lt;br /&gt;
|[[FIle: momentum_h2_mep_01533249.png|300px]]&lt;br /&gt;
|[[FIle: momentum_h2_dyn_01533249.png|300px]] &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280 || reactive || The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. Initially the molecule bond doesn&#039;t oscillate however after the reaction it does. || [[File:cp_table_1_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077 || unreactive || The atom and molecule don&#039;t have sufficient energy to overcome to reach the transition state so the H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; just reflects and returns to the reactants (the sign of its momentum changes)|| [[File:cp_table_2_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977 || reactive||  The atom and molecule have the correct amount of momentum to react and have enough energy to overcome the TS energy barrier. The initial molecule in this case has enough energy to vibrate. || [[File:cp_table_3_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || unreactive|| The atoms and molecule has an excess of energy they and react however the new formed molecule has so much energy that the bond vibrates to the point where it breaks and the initial reactants are formed again.|| [[File:cp_table_4_01533249.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477 || reactive || The atom and molecule react and the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond extends greatly but not to an extent that the bond breaks as in case 4 (above). The reaction pathway continues to the products vibrating greater than the case 1 and 3.|| [[File:cp_table_5_01533249.png|200px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The conclusion is that the sufficient momentum is required to reach the energy barrier of the transition state however and excess of momentum can result in the product having to much energy and the bond dissociating and the reactants forming again as in Case 4.&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The Transition state theory is that in order for reactants to turn into products they must first pass through a higher energy state form. One of the assumptions of transition state theory is that once reactants have passed  the transition state and the product has been formed they cannot revert back to the reactants. This rule is not followed in Case 4 (above), where the products are formed however they then reform the reactants. This would therefore result in an overestimate in the rate of the reaction of the as the product would be expected to form whereas in reality they are  not.&lt;br /&gt;
&#039;&#039;&#039;NEEDS A REFERENCE&#039;&#039;&#039;&lt;br /&gt;
another assumption is  transition state  theory is a classical theory and all the molecules behave in such way. Hence such effects such as quantum tunnelling are ignored, this would result in an understatement of the rates, however the effect is so small it isn&#039;t seen.&lt;br /&gt;
&lt;br /&gt;
==Exercise 2: F-H-H system ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The F+H2 reaction will be exothermic and the H+HF reaction will be endothermic. When looking at the surface plot it is clear that the H-F bond is at a lower energy compared to the H-H bond. The H-F bond is lower in energy due to the strength of the bond, H-F is a stronger bond due to the large difference in electronegativity of the atoms. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The approximate position of the transition state is r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 181 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 74.5 pm. (both momentums are set to zero).This was a point at which no reaction or movement occurs on the surface plot. It  can be confirmed by looking at the Internuclear Distances vs Time plot, where the gradients of he lines should be zero as the transition state is stable. &lt;br /&gt;
&lt;br /&gt;
[[File:Surface_Plot-hf-ts.png|400px|thumb|none| Surface Plot of transition state in F + H2 system.]]&lt;br /&gt;
&lt;br /&gt;
[[File:dist_vs_time_hf_ts.png|400px|thumb|none| Internuclear Distances vs Time plot of the transition state in a F + H2 System]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Activation energy&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The activation energy can calculated by looking at the Energy vs Time plot of a position offset of the transition state: in this case  r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 165 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the H+HF reaction is 126.17 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, values taken from figure 1 below.&lt;br /&gt;
&lt;br /&gt;
Activation energy =  -432.61 - (-558.78)&lt;br /&gt;
&lt;br /&gt;
The activation energy required for the H2 + F reaction is 2.41 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy = -433.64 - (-436.05)&lt;br /&gt;
&lt;br /&gt;
[[FIle:energy-hf-ae-01533249.png|400px|thumb|none| Figure 1: Energy vs Time plot offset the transition state.]]&lt;br /&gt;
&lt;br /&gt;
===Reaction Dynamics ===&lt;br /&gt;
&#039;&#039;&#039; In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial geometry required for a trajectory is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 175 pm and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; is 80 pm, and the momentums are p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;  and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. The energy released from the formation of the low energy H-F bond is conserved in the vibrating (K.E. energy) of the H-F bond, this can be seen in a Momentum vs Time plot, where after the reaction there is an oscillating motion in the change of momentum of F-H bond (blue line).&lt;/div&gt;</summary>
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