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	<updated>2026-05-17T05:36:41Z</updated>
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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776726</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776726"/>
		<updated>2019-05-10T16:58:30Z</updated>

		<summary type="html">&lt;p&gt;Cca17: /* Exercise 1 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The reactants do not possess enough energy to go through the transition state into the products.&lt;br /&gt;
Therefore the trajectory falls back down the surface towards the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic9.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic10.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants.&lt;br /&gt;
[[File:cca17pic11.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants. &lt;br /&gt;
It still possesses enough energy to overcome the transition state, so the trajectory goes into the products again at the end.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic12.png]]&lt;br /&gt;
|}&lt;br /&gt;
A higher momenta of the reactants does not always mean that the trajectory is reactive. If the initial momenta of the reactants are too high, the reactants could first form the products and then reform the reactants again as they have enough potential energy to overcome the activation energy and go through the transition state again to form the reactants.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;5. State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt;:&lt;br /&gt;
# Quantum-tunneling effects are assumed negligible and the Born-Oppenheimer approximation is invoked&lt;br /&gt;
# Atoms in the reactant state have energies that are Boltzmann distributed&lt;br /&gt;
# Once the system attains the transition state, with a velocity towards the product configuration, it will not reenter the initial state region again&lt;br /&gt;
The prediction by Transition Theory could predict a higher rate of reaction as potential backward reaction is not considered.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|[[File:cca17pic14.png|thumb|left|A reactive trajectory in which r(AB) = 2, r(BC) = 0.74, AB m= -1.5, BC m= 0]][[File:cca17pic13.png|thumb|left|Energy of the system over time]]&lt;br /&gt;
|&lt;br /&gt;
The kinetic energy of the system increases and the potential energy of the system decreases to the same degree as the reactants react to form products - which justifies that energy is conserved.This is also confirmed by the fact that the overall energy remains the same over time on the graph.&lt;br /&gt;
&lt;br /&gt;
The increase in kinetic energy could be confirmed experimentally by measuring the temperature of the reaction.&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|[[File:cca17pic15.png|thumb|left|High translational energy&lt;br /&gt;
A reactive trajectory in which r(AB) = 2, r(BC) = 1, AB m= -7, BC m= -1&lt;br /&gt;
]]&lt;br /&gt;
[[File:cca17pic16.png|thumb|left|High vibrational energy&lt;br /&gt;
A reactive trajectory in which r(AB) = 2, r(BC) = 1, AB m= -1.1, BC m= 6.5&lt;br /&gt;
]]&lt;br /&gt;
|&lt;br /&gt;
Polanyi&#039;s empirical rules states that vibration is more effective to promote the reaction than translation for late transition states.&lt;br /&gt;
&lt;br /&gt;
As the transition state is late, it is easier to reach the transition state by having a high vibrational energy than high translational energy,which is confirmed by the reaction trajectories on the left.&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
== References ==&lt;br /&gt;
  &amp;lt;references&amp;gt;&lt;br /&gt;
  &amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;T.Bligaard, J.K.Nørskov, in Chemical Bonding at Surfaces and Interfaces, Elsevier, Amsterdam, 2008, pp 255-321.&amp;lt;/ref&amp;gt;&lt;br /&gt;
  &amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776695</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776695"/>
		<updated>2019-05-10T16:54:30Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The reactants do not possess enough energy to go through the transition state into the products.&lt;br /&gt;
Therefore the trajectory falls back down the surface towards the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic9.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic10.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants.&lt;br /&gt;
[[File:cca17pic11.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants. &lt;br /&gt;
It still possesses enough energy to overcome the transition state, so the trajectory goes into the products again at the end.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic12.png]]&lt;br /&gt;
|}&lt;br /&gt;
A higher momenta of the reactants does not always mean that the trajectory is reactive. If the initial momenta of the reactants are too high, the reactants could first form the products and then reform the reactants again as they have enough potential energy to overcome the activation energy and go through the transition state again to form the reactants.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;5. State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt;:&lt;br /&gt;
# Quantum-tunneling effects are assumed negligible and the Born-Oppenheimer approximation is invoked&lt;br /&gt;
# Atoms in the reactant state have energies that are Boltzmann distributed&lt;br /&gt;
# Once the system attains the transition state, with a velocity towards the product configuration, it will not reenter the initial state region again&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|[[File:cca17pic14.png|thumb|left|A reactive trajectory in which r(AB) = 2, r(BC) = 0.74, AB m= -1.5, BC m= 0]][[File:cca17pic13.png|thumb|left|Energy of the system over time]]&lt;br /&gt;
|&lt;br /&gt;
The kinetic energy of the system increases and the potential energy of the system decreases to the same degree as the reactants react to form products - which justifies that energy is conserved.This is also confirmed by the fact that the overall energy remains the same over time on the graph.&lt;br /&gt;
&lt;br /&gt;
The increase in kinetic energy could be confirmed experimentally by measuring the temperature of the reaction.&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|[[File:cca17pic15.png|thumb|left|High translational energy&lt;br /&gt;
A reactive trajectory in which r(AB) = 2, r(BC) = 1, AB m= -7, BC m= -1&lt;br /&gt;
]]&lt;br /&gt;
[[File:cca17pic16.png|thumb|left|High vibrational energy&lt;br /&gt;
A reactive trajectory in which r(AB) = 2, r(BC) = 1, AB m= -1.1, BC m= 6.5&lt;br /&gt;
]]&lt;br /&gt;
|&lt;br /&gt;
Polanyi&#039;s empirical rules states that vibration is more effective to promote the reaction than translation for late transition states.&lt;br /&gt;
&lt;br /&gt;
As the transition state is late, it is easier to reach the transition state by having a high vibrational energy than high translational energy,which is confirmed by the reaction trajectories on the left.&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
== References ==&lt;br /&gt;
  &amp;lt;references&amp;gt;&lt;br /&gt;
  &amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;T.Bligaard, J.K.Nørskov, in Chemical Bonding at Surfaces and Interfaces, Elsevier, Amsterdam, 2008, pp 255-321.&amp;lt;/ref&amp;gt;&lt;br /&gt;
  &amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776642</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776642"/>
		<updated>2019-05-10T16:47:32Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The reactants do not possess enough energy to go through the transition state into the products.&lt;br /&gt;
Therefore the trajectory falls back down the surface towards the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic9.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic10.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants.&lt;br /&gt;
[[File:cca17pic11.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants. &lt;br /&gt;
It still possesses enough energy to overcome the transition state, so the trajectory goes into the products again at the end.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic12.png]]&lt;br /&gt;
|}&lt;br /&gt;
A higher momenta of the reactants does not always mean that the trajectory is reactive. If the initial momenta of the reactants are too high, the reactants could first form the products and then reform the reactants again as they have enough potential energy to overcome the activation energy and go through the transition state again to form the reactants.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;5. State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt;:&lt;br /&gt;
# Quantum-tunneling effects are assumed negligible and the Born-Oppenheimer approximation is invoked&lt;br /&gt;
# Atoms in the reactant state have energies that are Boltzmann distributed&lt;br /&gt;
# Once the system attains the transition state, with a velocity towards the product configuration, it will not reenter the initial state region again&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic14.png|thumb|left|A reactive trajectory in which r(AB) = 2, r(BC) = 0.74, AB m= -1.5, BC m= 0]][[File:cca17pic13.png|thumb|left|Energy of the system over time]]&lt;br /&gt;
|&lt;br /&gt;
The kinetic energy of the system increases and the potential energy of the system decreases to the same degree as the reactants react to form products - which justifies that energy is conserved.This is also confirmed by the fact that the overall energy remains the same over time on the graph.&lt;br /&gt;
&lt;br /&gt;
The increase in kinetic energy could be confirmed experimentally by measuring the temperature of the reaction.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic15.png|thumb|left|High translational energy]]&lt;br /&gt;
[[File:cca17pic16.png|thumb|left|High vibrational energy]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
== References ==&lt;br /&gt;
  &amp;lt;references&amp;gt;&lt;br /&gt;
  &amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;T.Bligaard, J.K.Nørskov, in Chemical Bonding at Surfaces and Interfaces, Elsevier, Amsterdam, 2008, pp 255-321.&amp;lt;/ref&amp;gt;&lt;br /&gt;
  &amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic16.png&amp;diff=776626</id>
		<title>File:Cca17pic16.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic16.png&amp;diff=776626"/>
		<updated>2019-05-10T16:46:19Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic15.png&amp;diff=776624</id>
		<title>File:Cca17pic15.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic15.png&amp;diff=776624"/>
		<updated>2019-05-10T16:46:00Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776477</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776477"/>
		<updated>2019-05-10T16:27:55Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The reactants do not possess enough energy to go through the transition state into the products.&lt;br /&gt;
Therefore the trajectory falls back down the surface towards the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic9.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic10.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants.&lt;br /&gt;
[[File:cca17pic11.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants. &lt;br /&gt;
It still possesses enough energy to overcome the transition state, so the trajectory goes into the products again at the end.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic12.png]]&lt;br /&gt;
|}&lt;br /&gt;
A higher momenta of the reactants does not always mean that the trajectory is reactive. If the initial momenta of the reactants are too high, the reactants could first form the products and then reform the reactants again as they have enough potential energy to overcome the activation energy and go through the transition state again to form the reactants.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;5. State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt;:&lt;br /&gt;
# Quantum-tunneling effects are assumed negligible and the Born-Oppenheimer approximation is invoked&lt;br /&gt;
# Atoms in the reactant state have energies that are Boltzmann distributed&lt;br /&gt;
# Once the system attains the transition state, with a velocity towards the product configuration, it will not reenter the initial state region again&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic14.png|thumb|left|A reactive trajectory in which r(AB) = 2, r(BC) = 0.74, AB m= -1.5, BC m= 0]][[File:cca17pic13.png|thumb|left|Energy of the system over time]]&lt;br /&gt;
|&lt;br /&gt;
The kinetic energy of the system increases and the potential energy of the system decreases to the same degree as the reactants react to form products - which justifies that energy is conserved.This is also confirmed by the fact that the overall energy remains the same over time on the graph.&lt;br /&gt;
&lt;br /&gt;
The increase in kinetic energy could be confirmed experimentally by measuring the temperature of the reaction.&lt;br /&gt;
|}&lt;br /&gt;
== References ==&lt;br /&gt;
  &amp;lt;references&amp;gt;&lt;br /&gt;
  &amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;T.Bligaard, J.K.Nørskov, in Chemical Bonding at Surfaces and Interfaces, Elsevier, Amsterdam, 2008, pp 255-321.&amp;lt;/ref&amp;gt;&lt;br /&gt;
  &amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776470</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776470"/>
		<updated>2019-05-10T16:26:49Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The reactants do not possess enough energy to go through the transition state into the products.&lt;br /&gt;
Therefore the trajectory falls back down the surface towards the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic9.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic10.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants.&lt;br /&gt;
[[File:cca17pic11.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants. &lt;br /&gt;
It still possesses enough energy to overcome the transition state, so the trajectory goes into the products again at the end.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic12.png]]&lt;br /&gt;
|}&lt;br /&gt;
A higher momenta of the reactants does not always mean that the trajectory is reactive. If the initial momenta of the reactants are too high, the reactants could first form the products and then reform the reactants again as they have enough potential energy to overcome the activation energy and go through the transition state again to form the reactants.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;5. State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt;:&lt;br /&gt;
# Quantum-tunneling effects are assumed negligible and the Born-Oppenheimer approximation is invoked&lt;br /&gt;
# Atoms in the reactant state have energies that are Boltzmann distributed&lt;br /&gt;
# Once the system attains the transition state, with a velocity towards the product configuration, it will not reenter the initial state region again&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic13.png|thumb|left|A reactive trajectory in which r(AB) = 2, r(BC) = 0.74, AB m= -1.5, BC m= 0]]&lt;br /&gt;
[[File:cca17pic14.png|thumb|left|Energy of the system over time]]&lt;br /&gt;
|&lt;br /&gt;
The kinetic energy of the system increases and the potential energy of the system decreases to the same degree as the reactants react to form products - which justifies that energy is conserved.This is also confirmed by the fact that the overall energy remains the same over time on the graph.&lt;br /&gt;
&lt;br /&gt;
The increase in kinetic energy could be confirmed experimentally by measuring the temperature of the reaction.&lt;br /&gt;
|}&lt;br /&gt;
== References ==&lt;br /&gt;
  &amp;lt;references&amp;gt;&lt;br /&gt;
  &amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;T.Bligaard, J.K.Nørskov, in Chemical Bonding at Surfaces and Interfaces, Elsevier, Amsterdam, 2008, pp 255-321.&amp;lt;/ref&amp;gt;&lt;br /&gt;
  &amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776463</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776463"/>
		<updated>2019-05-10T16:25:18Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The reactants do not possess enough energy to go through the transition state into the products.&lt;br /&gt;
Therefore the trajectory falls back down the surface towards the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic9.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic10.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants.&lt;br /&gt;
[[File:cca17pic11.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants. &lt;br /&gt;
It still possesses enough energy to overcome the transition state, so the trajectory goes into the products again at the end.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic12.png]]&lt;br /&gt;
|}&lt;br /&gt;
A higher momenta of the reactants does not always mean that the trajectory is reactive. If the initial momenta of the reactants are too high, the reactants could first form the products and then reform the reactants again as they have enough potential energy to overcome the activation energy and go through the transition state again to form the reactants.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;5. State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt;:&lt;br /&gt;
# Quantum-tunneling effects are assumed negligible and the Born-Oppenheimer approximation is invoked&lt;br /&gt;
# Atoms in the reactant state have energies that are Boltzmann distributed&lt;br /&gt;
# Once the system attains the transition state, with a velocity towards the product configuration, it will not reenter the initial state region again&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&amp;lt;/u&amp;gt;&lt;br /&gt;
[[File:cca17pic13.png|thumb|left|A reactive trajectory in which r(AB) = 2, r(BC) = 0.74, AB m= -1.5, BC m= 0]]&lt;br /&gt;
[[File:cca17pic14.png|thumb|left|Energy of the system over time]]&lt;br /&gt;
&lt;br /&gt;
The kinetic energy of the system increases and the potential energy of the system decreases to the same degree as the reactants react to form products - which justifies that energy is conserved.This is also confirmed by the fact that the overall energy remains the same over time on the graph.&lt;br /&gt;
&lt;br /&gt;
The increase in kinetic energy could be confirmed experimentally by measuring the temperature of the reaction.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
  &amp;lt;references&amp;gt;&lt;br /&gt;
  &amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;T.Bligaard, J.K.Nørskov, in Chemical Bonding at Surfaces and Interfaces, Elsevier, Amsterdam, 2008, pp 255-321.&amp;lt;/ref&amp;gt;&lt;br /&gt;
  &amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic14.png&amp;diff=776443</id>
		<title>File:Cca17pic14.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic14.png&amp;diff=776443"/>
		<updated>2019-05-10T16:21:54Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic13.png&amp;diff=776433</id>
		<title>File:Cca17pic13.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic13.png&amp;diff=776433"/>
		<updated>2019-05-10T16:20:17Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776429</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776429"/>
		<updated>2019-05-10T16:19:59Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The reactants do not possess enough energy to go through the transition state into the products.&lt;br /&gt;
Therefore the trajectory falls back down the surface towards the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic9.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic10.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants.&lt;br /&gt;
[[File:cca17pic11.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants. &lt;br /&gt;
It still possesses enough energy to overcome the transition state, so the trajectory goes into the products again at the end.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic12.png]]&lt;br /&gt;
|}&lt;br /&gt;
A higher momenta of the reactants does not always mean that the trajectory is reactive. If the initial momenta of the reactants are too high, the reactants could first form the products and then reform the reactants again as they have enough potential energy to overcome the activation energy and go through the transition state again to form the reactants.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;5. State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt;:&lt;br /&gt;
# Quantum-tunneling effects are assumed negligible and the Born-Oppenheimer approximation is invoked&lt;br /&gt;
# Atoms in the reactant state have energies that are Boltzmann distributed&lt;br /&gt;
# Once the system attains the transition state, with a velocity towards the product configuration, it will not reenter the initial state region again&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The kinetic energy of the system increases and the potential energy of the system decreases to the same degree as the reactants react to form products - which justifies that energy is conserved.&lt;br /&gt;
&lt;br /&gt;
The increase in kinetic energy could be confirmed experimentally by measuring the temperature of the reaction.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
  &amp;lt;references&amp;gt;&lt;br /&gt;
  &amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;T.Bligaard, J.K.Nørskov, in Chemical Bonding at Surfaces and Interfaces, Elsevier, Amsterdam, 2008, pp 255-321.&amp;lt;/ref&amp;gt;&lt;br /&gt;
  &amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776388</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776388"/>
		<updated>2019-05-10T16:14:20Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The reactants do not possess enough energy to go through the transition state into the products.&lt;br /&gt;
Therefore the trajectory falls back down the surface towards the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic9.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic10.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants.&lt;br /&gt;
[[File:cca17pic11.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants. &lt;br /&gt;
It still possesses enough energy to overcome the transition state, so the trajectory goes into the products again at the end.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic12.png]]&lt;br /&gt;
|}&lt;br /&gt;
A higher momenta of the reactants does not always mean that the trajectory is reactive. If the initial momenta of the reactants are too high, the reactants could first form the products and then reform the reactants again as they have enough potential energy to overcome the activation energy and go through the transition state again to form the reactants.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;5. State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Assumptions &amp;lt;ref name=&amp;quot;TS&amp;quot;/&amp;gt;:&lt;br /&gt;
# Quantum-tunneling effects are assumed negligible and the Born-Oppenheimer approximation is invoked&lt;br /&gt;
# Atoms in the reactant state have energies that are Boltzmann distributed&lt;br /&gt;
# Once the system attains the transition state, with a velocity towards the product configuration, it will not reenter the initial state region again&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
  &amp;lt;references&amp;gt;&lt;br /&gt;
  &amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt;T.Bligaard, J.K.Nørskov, in Chemical Bonding at Surfaces and Interfaces, Elsevier, Amsterdam, 2008, pp 255-321.&amp;lt;/ref&amp;gt;&lt;br /&gt;
  &amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776336</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776336"/>
		<updated>2019-05-10T16:04:40Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The reactants do not possess enough energy to go through the transition state into the products.&lt;br /&gt;
Therefore the trajectory falls back down the surface towards the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic9.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic10.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants.&lt;br /&gt;
[[File:cca17pic11.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants. &lt;br /&gt;
It still possesses enough energy to overcome the transition state, so the trajectory goes into the products again at the end.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic12.png]]&lt;br /&gt;
|}&lt;br /&gt;
A higher momenta of the reactants does not always mean that the trajectory is reactive. If the initial momenta of the reactants are too high, the reactants could first form the products and then reform the reactants again as they have enough potential energy to overcome the activation energy and go through the transition state again to form the reactants.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;5. State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Assumptions &amp;lt;nowiki&amp;gt;&amp;lt;ref name=&amp;quot;TS&amp;quot; /&amp;gt;&amp;lt;/nowiki&amp;gt;:&lt;br /&gt;
# Quantum-tunneling effects are assumed negligible and the Born-Oppenheimer approximation is invoked&lt;br /&gt;
# Atoms in the reactant state have energies that are Boltzmann distributed&lt;br /&gt;
# Once the system attains the transition state, with a velocity towards the product configuration, it will not reenter the initial state region again&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
 &amp;lt;nowiki&amp;gt;&amp;lt;references&amp;gt;&lt;br /&gt;
  &amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt; T.Bligaard, J.K.Nørskov, in Chemical Bonding at Surfaces and Interfaces, Elsevier, Amsterdam, 2008, pp255-321.&amp;lt;/ref&amp;gt;&lt;br /&gt;
  &amp;lt;/references&amp;gt;&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776324</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776324"/>
		<updated>2019-05-10T16:03:28Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The reactants do not possess enough energy to go through the transition state into the products.&lt;br /&gt;
Therefore the trajectory falls back down the surface towards the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic9.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic10.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants.&lt;br /&gt;
[[File:cca17pic11.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants. &lt;br /&gt;
It still possesses enough energy to overcome the transition state, so the trajectory goes into the products again at the end.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic12.png]]&lt;br /&gt;
|}&lt;br /&gt;
A higher momenta of the reactants does not always mean that the trajectory is reactive. If the initial momenta of the reactants are too high, the reactants could first form the products and then reform the reactants again as they have enough potential energy to overcome the activation energy and go through the transition state again to form the reactants.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;5. State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Assumptions &amp;lt;nowiki&amp;gt;&amp;lt;ref name=&amp;quot;TS&amp;quot; /&amp;gt;&amp;lt;/nowiki&amp;gt;:&lt;br /&gt;
# Quantum-tunneling effects are assumed negligible and the Born-Oppenheimer approximation is invoked&lt;br /&gt;
# Atoms in the reactant state have energies that are Boltzmann distributed&lt;br /&gt;
# Once the system attains the transition state, with a velocity towards the product configuration, it will not reenter the initial state region again&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
 &amp;lt;nowiki&amp;gt;&amp;lt;references&amp;gt;&lt;br /&gt;
 &amp;lt;ref name=&amp;quot;TS&amp;quot;&amp;gt; T.Bligaard, J.K.Nørskov, in Chemical Bonding at Surfaces and Interfaces, Elsevier, Amsterdam,, vol. 1, ch. 4, pp. 253–255.&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &amp;lt;/references&amp;gt;&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776138</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776138"/>
		<updated>2019-05-10T15:41:23Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The reactants do not possess enough energy to go through the transition state into the products.&lt;br /&gt;
Therefore the trajectory falls back down the surface towards the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic9.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes through the transition state and into the products as the reactants possess the right amount of energy for the forward reaction to occur.&lt;br /&gt;
[[File:cca17pic10.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants.&lt;br /&gt;
[[File:cca17pic11.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|The trajectory goes from the reactants into the products initially, but possesses enough energy and hence goes back towards the reactants. &lt;br /&gt;
It still possesses enough energy to overcome the transition state, so the trajectory goes into the products again at the end.&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic12.png]]&lt;br /&gt;
|}&lt;br /&gt;
A higher momenta of the reactants does not always mean that the trajectory is reactive. If the initial momenta of the reactants are too high, the reactants could first form the products and then reform the reactants again as they have enough potential energy to overcome the activation energy and go through the transition state again to form the reactants.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776062</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776062"/>
		<updated>2019-05-10T15:31:37Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|[[File:cca17pic9.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|[[File:cca17pic10.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|[[File:cca17pic11.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|[[File:cca17pic12.png]]&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic12.png&amp;diff=776052</id>
		<title>File:Cca17pic12.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic12.png&amp;diff=776052"/>
		<updated>2019-05-10T15:30:45Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic11.png&amp;diff=776046</id>
		<title>File:Cca17pic11.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic11.png&amp;diff=776046"/>
		<updated>2019-05-10T15:30:19Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic10.png&amp;diff=776044</id>
		<title>File:Cca17pic10.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic10.png&amp;diff=776044"/>
		<updated>2019-05-10T15:29:58Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic9.png&amp;diff=776041</id>
		<title>File:Cca17pic9.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic9.png&amp;diff=776041"/>
		<updated>2019-05-10T15:29:25Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776011</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776011"/>
		<updated>2019-05-10T15:25:42Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
[[File:cca17pic8.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776007</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=776007"/>
		<updated>2019-05-10T15:25:17Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
[[File:cca17pic8.png|thumb|left|]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic8.png&amp;diff=775975</id>
		<title>File:Cca17pic8.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic8.png&amp;diff=775975"/>
		<updated>2019-05-10T15:21:21Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775724</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775724"/>
		<updated>2019-05-10T14:50:12Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic6.png|thumb|left|Transition state position for the exothermic reaction]]&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic7.png|thumb|left|Transition state position for the endothermic reaction]]&lt;br /&gt;
|}&lt;br /&gt;
The transition state is located at the internuclear distances at which there is no reaction trajectory and stays that the point.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775707</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775707"/>
		<updated>2019-05-10T14:48:08Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic6.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
[[File:cca17pic7.png|thumb|left|Activation energy for the endothermic reaction]]&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic7.png&amp;diff=775704</id>
		<title>File:Cca17pic7.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic7.png&amp;diff=775704"/>
		<updated>2019-05-10T14:47:42Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic6.png&amp;diff=775701</id>
		<title>File:Cca17pic6.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic6.png&amp;diff=775701"/>
		<updated>2019-05-10T14:47:22Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775684</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775684"/>
		<updated>2019-05-10T14:45:06Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.815&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
r(AB) = 0.74&lt;br /&gt;
&lt;br /&gt;
r(BC) = 1.815&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.89&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
Activation Energy = -103.756 - (-104.015) = 0.259 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|H + HF&lt;br /&gt;
&lt;br /&gt;
r(AB) = 1.805&lt;br /&gt;
&lt;br /&gt;
r(BC) = 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|Activation Energy = -103.687 - (-133.789) = 30.102 kcal mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775636</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775636"/>
		<updated>2019-05-10T14:39:26Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.815&lt;br /&gt;
&lt;br /&gt;
BC 0.7399&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.74&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.89&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
AE = -103.756 - (-104.015) = 0.259 kcal mol-1&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 1.805&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|AE = -103.687 - (-133.789) = 30.102 kcal mol-1&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775605</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775605"/>
		<updated>2019-05-10T14:36:04Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.815&lt;br /&gt;
&lt;br /&gt;
BC 0.7399&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.74&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.89&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for the exothermic reaction]]&lt;br /&gt;
|&lt;br /&gt;
AE = -103.756 - (-104.015) = 0.259 kcal mol-1&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 1.805&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic5.png|thumb|left|Activation energy for the endothermic reaction]]&lt;br /&gt;
|AE = -103.687 - (-133.789) = 30.102 kcal mol-1&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic4.png&amp;diff=775585</id>
		<title>File:Cca17pic4.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic4.png&amp;diff=775585"/>
		<updated>2019-05-10T14:34:35Z</updated>

		<summary type="html">&lt;p&gt;Cca17: Cca17 uploaded a new version of File:Cca17pic4.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775575</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775575"/>
		<updated>2019-05-10T14:33:53Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.815&lt;br /&gt;
&lt;br /&gt;
BC 0.7399&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.74&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.89&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
|[[File:cca17pic3.png|thumb|left|Activation energy for ]]&lt;br /&gt;
|&lt;br /&gt;
AE = -103.756 - (-104.015) = 0.259 kcal mol-1&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 1.805&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= 0&lt;br /&gt;
|[[File:cca17pic4.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|AE = -103.687 - (-133.789) = 30.102 kcal mol-1&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775087</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775087"/>
		<updated>2019-05-10T13:40:48Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.815&lt;br /&gt;
&lt;br /&gt;
BC 0.7399&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.74&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.89&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|&lt;br /&gt;
&lt;br /&gt;
AE = -103.756 - (-104.015) = 0.259&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.75&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|AE = -103.739 - (-104.009) = 0.27&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic3.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
[[File:cca17pic4.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic4.png&amp;diff=775080</id>
		<title>File:Cca17pic4.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic4.png&amp;diff=775080"/>
		<updated>2019-05-10T13:40:00Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic3.png&amp;diff=775073</id>
		<title>File:Cca17pic3.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic3.png&amp;diff=775073"/>
		<updated>2019-05-10T13:39:41Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775045</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775045"/>
		<updated>2019-05-10T13:34:08Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(ABC)&#039;&#039;&#039;r(AB) 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.815&lt;br /&gt;
&lt;br /&gt;
BC 0.7399&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is exothermic as it proceeds from the reactants which are at a high potential energy to the products of low potential energy. Therefore energy is released during the process making it an exothermic reaction.&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.74&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|The reaction is endothermic it proceeds from the reactants which are at a low potential energy to the products of highpotential energy. Therefore energy is taken in during the process making it an exothermic reaction.&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;u&amp;gt;Report the activation energy for both reactions.&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.89&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the exothermic reaction on a potential energy surface.]]&lt;br /&gt;
|&lt;br /&gt;
&lt;br /&gt;
AE = -103.756 - (-104.015) = 0.259&lt;br /&gt;
|-&lt;br /&gt;
|H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.75&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
|[[File:cca17pic2.png|thumb|left|Trajectory of the endothermic reaction on a potential energy surface.]]&lt;br /&gt;
|AE = -103.739 - (-104.009) = 0.27&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775007</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=775007"/>
		<updated>2019-05-10T13:28:53Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​) , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&#039;&#039;&#039;r(AB) 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|Trajectory of the reaction on a potential energy surface.]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.815&lt;br /&gt;
&lt;br /&gt;
BC 0.7399&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.74&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.89&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
AE = -103.756 - (-104.015) = 0.259&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.75&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
AE = -103.739 - (-104.009) = 0.27&lt;br /&gt;
&lt;br /&gt;
[[File:cca17pic2.png|thumb|left|Trajectory of the reaction on a potential energy surface.]]&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic2.png&amp;diff=774974</id>
		<title>File:Cca17pic2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic2.png&amp;diff=774974"/>
		<updated>2019-05-10T13:24:09Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=774965</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=774965"/>
		<updated>2019-05-10T13:23:01Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|&#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (ABC)&#039;&#039;&#039;r(AB) 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) 0.74&lt;br /&gt;
&lt;br /&gt;
AB m= 0&lt;br /&gt;
&lt;br /&gt;
BC m= -1.5&lt;br /&gt;
|[[File:cca17pic1.png|thumb|left|text-bottom|A Gaussview image of an optimised benzene molecule.]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&#039;&#039;&#039;H + HF (ABC)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.815&lt;br /&gt;
&lt;br /&gt;
BC 0.7399&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.74&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.89&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
AE = -103.756 - (-104.015) = 0.259&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.75&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
AE = -103.739 - (-104.009) = 0.27&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=774863</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=774863"/>
		<updated>2019-05-10T13:05:46Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -1.5&lt;br /&gt;
[[File:cca17pic1.png|thumb|left|text-bottom|A Gaussview image of an optimised benzene molecule.]]&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.815&lt;br /&gt;
&lt;br /&gt;
BC 0.7399&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.74&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.89&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
AE = -103.756 - (-104.015) = 0.259&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.75&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
AE = -103.739 - (-104.009) = 0.27&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic1.png&amp;diff=774835</id>
		<title>File:Cca17pic1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Cca17pic1.png&amp;diff=774835"/>
		<updated>2019-05-10T13:00:06Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=774791</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=774791"/>
		<updated>2019-05-10T12:52:52Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory. It is also the specific combination of internuclear distances AB and BC at which the trajectory is a point on the contour plot.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant, where a local minimum will give H &amp;gt; 0.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
r(AB) 1.5&lt;br /&gt;
&lt;br /&gt;
r(BC) 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -1.5&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.815&lt;br /&gt;
&lt;br /&gt;
BC 0.7399&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.74&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.89&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
AE = -103.756 - (-104.015) = 0.259&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.75&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
AE = -103.739 - (-104.009) = 0.27&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=774777</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=774777"/>
		<updated>2019-05-10T12:49:29Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
Report the activation energy for both reactions.&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -1.5&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.815&lt;br /&gt;
&lt;br /&gt;
BC 0.7399&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.74&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.89&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
AE = -103.756 - (-104.015) = 0.259&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.75&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
AE = -103.739 - (-104.009) = 0.27&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=774776</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=774776"/>
		<updated>2019-05-10T12:49:03Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
Report the activation energy for both reactions.&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is located at the saddle point in the potential energy surface diagram, hence it is mathematically defined as : ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 and H &amp;lt; 0, where H = f&amp;lt;sub&amp;gt;rr&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)f&amp;lt;sub&amp;gt;VV&amp;lt;/sub&amp;gt;(r&amp;lt;sub&amp;gt;0​&amp;lt;/sub&amp;gt;,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)−f&amp;lt;sub&amp;gt;rV&amp;lt;/sub&amp;gt;​(r&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​,V&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;​)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; , which is the determinant of the second partial derivative at the  &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -1.5&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.815&lt;br /&gt;
&lt;br /&gt;
BC 0.7399&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.74&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.89&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
AE = -103.756 - (-104.015) = 0.259&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.75&lt;br /&gt;
&lt;br /&gt;
BC 1.8136&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
AE = -103.739 - (-104.009) = 0.27&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=773307</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=773307"/>
		<updated>2019-05-09T16:08:01Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as:&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{\delta V(r_i)}{\delta r_i}=0 &amp;lt;/math&amp;gt; and &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -1.5&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;br /&gt;
&lt;br /&gt;
-&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.815&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 0.74&lt;br /&gt;
&lt;br /&gt;
BC 1.8135&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m 0&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=772623</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=772623"/>
		<updated>2019-05-09T14:34:58Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as:&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{\delta V(r_i)}{\delta r_i}=0 &amp;lt;/math&amp;gt; and &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;br /&gt;
&lt;br /&gt;
Exercise 2&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;Locate the approximate position of the transition state.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2 (ABC)&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.74&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -1.5&lt;br /&gt;
&lt;br /&gt;
H + HF (ABC)&lt;br /&gt;
&lt;br /&gt;
AB 1.5&lt;br /&gt;
&lt;br /&gt;
BC 0.92&lt;br /&gt;
&lt;br /&gt;
AB m 0&lt;br /&gt;
&lt;br /&gt;
BC m -10&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=769816</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=769816"/>
		<updated>2019-05-07T15:58:24Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as:&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{\delta V(r_i)}{\delta r_i}=0 &amp;lt;/math&amp;gt; and &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive.&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=769748</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=769748"/>
		<updated>2019-05-07T15:51:35Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;u&amp;gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as:&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{\delta V(r_i)}{\delta r_i}=0 &amp;lt;/math&amp;gt; and &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&amp;lt;/u&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24 at large t.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 3.5 and the average momenta  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 1.24, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) = 2.48 at large t.&lt;br /&gt;
&lt;br /&gt;
Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed. - the molecule and the atom coming together instead of moving apart.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;u&amp;gt;4.Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?&amp;lt;/u&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|goes through the transition state and into the products&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=769329</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=769329"/>
		<updated>2019-05-07T15:13:00Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as:&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{\delta V(r_i)}{\delta r_i}=0 &amp;lt;/math&amp;gt; and &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant.&lt;br /&gt;
&lt;br /&gt;
2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=0.74 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.907 Å.&lt;br /&gt;
&lt;br /&gt;
3.Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
The mep trajectory is a keeps the potential energy at the minimum in a straight line, whereas the dynamic trajectory is wavy does not always stay at the potential energy minimum.&lt;br /&gt;
&lt;br /&gt;
4.&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=769039</id>
		<title>Kjh68</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Kjh68&amp;diff=769039"/>
		<updated>2019-05-07T14:35:34Z</updated>

		<summary type="html">&lt;p&gt;Cca17: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;1. On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as:&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{\delta V(r_i)}{\delta r_i}=0 &amp;lt;/math&amp;gt; and &lt;br /&gt;
&lt;br /&gt;
The transition state can be identified by going along the minimum energy trajectory and locating the point at which potential energy is maximum along the trajectory.&lt;br /&gt;
&lt;br /&gt;
It could be distinguished from a local minimum of the potential by using the second partial derivative discriminant.&lt;br /&gt;
&lt;br /&gt;
2. Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
For a trajectory starting with r(AB)=r(BC)=2.3 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.0, the transition state occurs where the internuclear distance is approximately 0.57 Å.&lt;/div&gt;</summary>
		<author><name>Cca17</name></author>
	</entry>
</feed>