<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
	<id>https://chemwiki.ch.ic.ac.uk/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=Yz32918</id>
	<title>ChemWiki - User contributions [en]</title>
	<link rel="self" type="application/atom+xml" href="https://chemwiki.ch.ic.ac.uk/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=Yz32918"/>
	<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/wiki/Special:Contributions/Yz32918"/>
	<updated>2026-04-11T05:45:04Z</updated>
	<subtitle>User contributions</subtitle>
	<generator>MediaWiki 1.43.0</generator>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805973</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805973"/>
		<updated>2020-05-15T22:51:30Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) kJ mol^{-1} = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H F F system activation energy surface plot 1.png|thumb|center|400px|The surface plot of how the energy of the transition state of the H + H-F reaction goes back to the energy of the reactant calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system energy vs time plot 1.png|thumb|center|400px|The energy vs time plot of the H + H-F reaction going from the transition state to the reactant.]]&lt;br /&gt;
&lt;br /&gt;
=== Release of the reaction energy ===&lt;br /&gt;
&lt;br /&gt;
The total energy of the reaction is conserved, when the F atom and a H2 molecule collided with each other, the H2 atom will bounce back and forth between the F1 atom and the H3 atom, whether the reaction trajectory is reactive or not depends on how much the initial kinetic energy of the F atom and H2 molecule have and how far the H3 atom is bumping away from F1 and H2. Initially, the system composed of F1 atom and H2 molecule, there will be no change of dipole moment when the H2 molecule vibrates and is IR inactive. If the reaction path is reactive, the product will be a H atom and a H-F molecule. If the H-F molecule vibrates, there will be a change in dipole moment and therefore IR active. We could observe a band due to the transition from v0 to v1 vibrational state and 1st and 2nd overtunes of the vibration. So the release of reaction energy can be measured by IR spectroscopy. Also, when a molecule vibrates, it radiates energy in the range of IR and the radiation can be detected. Also, calorimetry can be used to monitor the reaction as the reaction is exothermic and temperature will increase. If the reaction trajectory is not reactive, the reactant will remain the same so it will not be IR reactive.&lt;br /&gt;
&lt;br /&gt;
==== Reactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system reactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of a reactive trajectory of the F + H2 system. The orange line represents the vibration of the H2 molecule at the start which is not IR active and th blue line represents the vibration of the H-F molecule formed, there is a change in dipole moment, it is IR active.]]&lt;br /&gt;
&lt;br /&gt;
==== Unreactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system unreactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of an unreactive trajectory. The orange line represents the vibration of the H2 molecule, there is no change in dipole moment, so it is not IR active. The product is not formed and the reaction stays the same. The product is still IR inactive.]]&lt;br /&gt;
&lt;br /&gt;
=== Distribution of energy, position of transition state ===&lt;br /&gt;
&lt;br /&gt;
The distribution of energy such as translational and vibrational energies between the atoms and molecules in a system is important to whether a reaction trajectory is reactive or not. If in the system there is little kinetic or vibrational energy, the atom cannot cross the transition state because it does not have enough energy. Once the system has enough energy, the distribution between translational, vibrational and potential energy is important. After a system have enough energy to overcome the activation energy barrier, the excess energy the system possess will allow the middle atom to bounce back and force between the first and the third atom. Whether the second atom will stay with the first or the third atom depends on how much excess energy it has and therefore determines whether a new bond will form or not. As the excess energy increases incrementally, whether the reaction trajectory is reactive or not alternates. As shown in the exercise, an F atom and a H2 molecule approaching each other with little translational energy but enough energy above the activation energy barrier can lead to the formation of the product. There is almost no vibrational energy, once the H2 atom is pulled towards the F1 atom, it stick with it and does not bounce back.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system 5 7 reactive contour plot.png|thumb|center|400px|The contour plot of the F + H2 system when p1 = - 1.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2 = - 5.7 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is a reactive trajectory. Whether a reaction trajectory is reactive or not changes constantly for momenta p2 around -6.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system 5 6 unreactive contour plot.png|thumb|center|400px|The contour plot of the F + H2 system when p1 = - 1.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2 = - 5.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is a unreactive trajectory. ]]&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules and Hammond&#039;s Postulate ====&lt;br /&gt;
&lt;br /&gt;
When the transition state of a reaction is not symmetric a in the case of F + H2 and H + H-F systems, the transition state will change its position. In the F + H2 system, the transition state is a early transition state, it is closer to the reactant than the product. Translational energy will make the reaction more efficient because it helps to go across the transition state In the H + H-F system, the transition state is a late transition state, the transition state is close to the product than the reactant. Vibrational energy in the reactant will increase the efficiency of the reaction as it helps to go beyond the transition state while a translational energy will bounce back. This rule is closely related to the Hammond&#039;s postulate in determining whether the transition state will be like the reactant or the product according to whether the reaction is exothermic or endothermic.&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
1. J. C. POLANYI, Science (80-. )., 1997, 236, 680–690.&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805965</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805965"/>
		<updated>2020-05-15T22:40:45Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) kJ mol^{-1} = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H F F system activation energy surface plot 1.png|thumb|center|400px|The surface plot of how the energy of the transition state of the H + H-F reaction goes back to the energy of the reactant calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system energy vs time plot 1.png|thumb|center|400px|The energy vs time plot of the H + H-F reaction going from the transition state to the reactant.]]&lt;br /&gt;
&lt;br /&gt;
=== Release of the reaction energy ===&lt;br /&gt;
&lt;br /&gt;
The total energy of the reaction is conserved, when the F atom and a H2 molecule collided with each other, the H2 atom will bounce back and forth between the F1 atom and the H3 atom, whether the reaction trajectory is reactive or not depends on how much the initial kinetic energy of the F atom and H2 molecule have and how far the H3 atom is bumping away from F1 and H2. Initially, the system composed of F1 atom and H2 molecule, there will be no change of dipole moment when the H2 molecule vibrates and is IR inactive. If the reaction path is reactive, the product will be a H atom and a H-F molecule. If the H-F molecule vibrates, there will be a change in dipole moment and therefore IR active. We could observe a band due to the transition from v0 to v1 vibrational state and 1st and 2nd overtunes of the vibration. So the release of reaction energy can be measured by IR spectroscopy. Also, when a molecule vibrates, it radiates energy in the range of IR and the radiation can be detected. Also, calorimetry can be used to monitor the reaction as the reaction is exothermic and temperature will increase. If the reaction trajectory is not reactive, the reactant will remain the same so it will not be IR reactive.&lt;br /&gt;
&lt;br /&gt;
==== Reactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system reactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of a reactive trajectory of the F + H2 system. The orange line represents the vibration of the H2 molecule at the start which is not IR active and th blue line represents the vibration of the H-F molecule formed, there is a change in dipole moment, it is IR active.]]&lt;br /&gt;
&lt;br /&gt;
==== Unreactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system unreactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of an unreactive trajectory. The orange line represents the vibration of the H2 molecule, there is no change in dipole moment, so it is not IR active. The product is not formed and the reaction stays the same. The product is still IR inactive.]]&lt;br /&gt;
&lt;br /&gt;
=== Distribution of energy, position of transition state ===&lt;br /&gt;
&lt;br /&gt;
The distribution of energy such as translational and vibrational energies between the atoms and molecules in a system is important to whether a reaction trajectory is reactive or not. If in the system there is little kinetic or vibrational energy, the atom cannot cross the transition state because it does not have enough energy. Once the system has enough energy, the distribution between translational, vibrational and potential energy is important. After a system have enough energy to overcome the activation energy barrier, the excess energy the system possess will allow the middle atom to bounce back and force between the first and the third atom. Whether the second atom will stay with the first or the third atom depends on how much excess energy it has and therefore determines whether a new bond will form or not. As the excess energy increases incrementally, whether the reaction trajectory is reactive or not alternates. As shown in the exercise, an F atom and a H2 molecule approaching each other with little translational energy but enough energy above the activation energy barrier can lead to the formation of the product. There is almost no vibrational energy, once the H2 atom is pulled towards the F1 atom, it stick with it and does not bounce back.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system 5 7 reactive contour plot.png|thumb|center|400px|The contour plot of the F + H2 system when p1 = - 1.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2 = - 5.7 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is a reactive trajectory. Whether a reaction trajectory is reactive or not changes constantly for momenta p2 around -6.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system 5 6 unreactive contour plot.png|thumb|center|400px|The contour plot of the F + H2 system when p1 = - 1.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2 = - 5.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is a unreactive trajectory. ]]&lt;br /&gt;
&lt;br /&gt;
==== Polanyi&#039;s empirical rules and Hammond&#039;s Postulate ====&lt;br /&gt;
&lt;br /&gt;
When the transition state of a reaction is not symmetric a in the case of F + H2 and H + H-F systems, the transition state will change its position. In the F + H2 system, the transition state is a early transition state, it is closer to the reactant than the product. Translational energy will make the reaction more efficient because it helps to go across the transition state In the H + H-F system, the transition state is a late transition state, the transition state is close to the product than the reactant. Vibrational energy in the reactant will increase the efficiency of the reaction as it helps to go beyond the transition state while a translational energy will bounce back. This rule is closely related to the Hammond&#039;s postulate in determining whether the transition state will be like the reactant or the product according to whether the reaction is exothermic or endothermic.&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805962</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805962"/>
		<updated>2020-05-15T22:39:22Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) kJ mol^{-1} = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H F F system activation energy surface plot 1.png|thumb|center|400px|The surface plot of how the energy of the transition state of the H + H-F reaction goes back to the energy of the reactant calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system energy vs time plot 1.png|thumb|center|400px|The energy vs time plot of the H + H-F reaction going from the transition state to the reactant.]]&lt;br /&gt;
&lt;br /&gt;
=== Release of the reaction energy ===&lt;br /&gt;
&lt;br /&gt;
The total energy of the reaction is conserved, when the F atom and a H2 molecule collided with each other, the H2 atom will bounce back and forth between the F1 atom and the H3 atom, whether the reaction trajectory is reactive or not depends on how much the initial kinetic energy of the F atom and H2 molecule have and how far the H3 atom is bumping away from F1 and H2. Initially, the system composed of F1 atom and H2 molecule, there will be no change of dipole moment when the H2 molecule vibrates and is IR inactive. If the reaction path is reactive, the product will be a H atom and a H-F molecule. If the H-F molecule vibrates, there will be a change in dipole moment and therefore IR active. We could observe a band due to the transition from v0 to v1 vibrational state and 1st and 2nd overtunes of the vibration. So the release of reaction energy can be measured by IR spectroscopy. Also, when a molecule vibrates, it radiates energy in the range of IR and the radiation can be detected. Also, calorimetry can be used to monitor the reaction as the reaction is exothermic and temperature will increase. If the reaction trajectory is not reactive, the reactant will remain the same so it will not be IR reactive.&lt;br /&gt;
&lt;br /&gt;
==== Reactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system reactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of a reactive trajectory of the F + H2 system. The orange line represents the vibration of the H2 molecule at the start which is not IR active and th blue line represents the vibration of the H-F molecule formed, there is a change in dipole moment, it is IR active.]]&lt;br /&gt;
&lt;br /&gt;
==== Unreactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system unreactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of an unreactive trajectory. The orange line represents the vibration of the H2 molecule, there is no change in dipole moment, so it is not IR active. The product is not formed and the reaction stays the same. The product is still IR inactive.]]&lt;br /&gt;
&lt;br /&gt;
=== Distribution of energy, position of transition state ===&lt;br /&gt;
&lt;br /&gt;
The distribution of energy such as translational and vibrational energies between the atoms and molecules in a system is important to whether a reaction trajectory is reactive or not. If in the system there is little kinetic or vibrational energy, the atom cannot cross the transition state because it does not have enough energy. Once the system has enough energy, the distribution between translational, vibrational and potential energy is important. After a system have enough energy to overcome the activation energy barrier, the excess energy the system possess will allow the middle atom to bounce back and force between the first and the third atom. Whether the second atom will stay with the first or the third atom depends on how much excess energy it has and therefore determines whether a new bond will form or not. As the excess energy increases incrementally, whether the reaction trajectory is reactive or not alternates. As shown in the exercise, an F atom and a H2 molecule approaching each other with little translational energy but enough energy above the activation energy barrier can lead to the formation of the product. There is almost no vibrational energy, once the H2 atom is pulled towards the F1 atom, it stick with it and does not bounce back.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system 5 7 reactive contour plot.png|thumb|center|400px|The contour plot of the F + H2 system when p1 = - 1.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2 = - 5.7 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is a reactive trajectory. Whether a reaction trajectory is reactive or not changes constantly for momenta p2 around -6.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system 5 6 unreactive contour plot.png|thumb|center|400px|The contour plot of the F + H2 system when p1 = - 1.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2 = - 5.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is a unreactive trajectory. ]]&lt;br /&gt;
&lt;br /&gt;
When the transition state of a reaction is not symmetric a in the case of F + H2 and H + H-F systems, the transition state will change its position. In the F + H2 system, the transition state is a early transition state, it is closer to the reactant than the product. Translational energy will make the reaction more efficient because it helps to go across the transition state In the H + H-F system, the transition state is a late transition state, the transition state is close to the product than the reactant. Vibrational energy in the reactant will increase the efficiency of the reaction as it helps to go beyond the transition state while a translational energy will bounce back. This rule is closely related to the Hammond&#039;s postulate in determining whether the transition state will be like the reactant or the product according to whether the reaction is exothermic or endothermic.&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805955</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805955"/>
		<updated>2020-05-15T22:30:50Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) kJ mol^{-1} = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H F F system activation energy surface plot 1.png|thumb|center|400px|The surface plot of how the energy of the transition state of the H + H-F reaction goes back to the energy of the reactant calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system energy vs time plot 1.png|thumb|center|400px|The energy vs time plot of the H + H-F reaction going from the transition state to the reactant.]]&lt;br /&gt;
&lt;br /&gt;
=== Release of the reaction energy ===&lt;br /&gt;
&lt;br /&gt;
The total energy of the reaction is conserved, when the F atom and a H2 molecule collided with each other, the H2 atom will bounce back and forth between the F1 atom and the H3 atom, whether the reaction trajectory is reactive or not depends on how much the initial kinetic energy of the F atom and H2 molecule have and how far the H3 atom is bumping away from F1 and H2. Initially, the system composed of F1 atom and H2 molecule, there will be no change of dipole moment when the H2 molecule vibrates and is IR inactive. If the reaction path is reactive, the product will be a H atom and a H-F molecule. If the H-F molecule vibrates, there will be a change in dipole moment and therefore IR active. We could observe a band due to the transition from v0 to v1 vibrational state and 1st and 2nd overtunes of the vibration. So the release of reaction energy can be measured by IR spectroscopy. Also, when a molecule vibrates, it radiates energy in the range of IR and the radiation can be detected. Also, calorimetry can be used to monitor the reaction as the reaction is exothermic and temperature will increase. If the reaction trajectory is not reactive, the reactant will remain the same so it will not be IR reactive.&lt;br /&gt;
&lt;br /&gt;
==== Reactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system reactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of a reactive trajectory of the F + H2 system. The orange line represents the vibration of the H2 molecule at the start which is not IR active and th blue line represents the vibration of the H-F molecule formed, there is a change in dipole moment, it is IR active.]]&lt;br /&gt;
&lt;br /&gt;
==== Unreactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system unreactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of an unreactive trajectory. The orange line represents the vibration of the H2 molecule, there is no change in dipole moment, so it is not IR active. The product is not formed and the reaction stays the same. The product is still IR inactive.]]&lt;br /&gt;
&lt;br /&gt;
=== Distribution of energy, position of transition state ===&lt;br /&gt;
&lt;br /&gt;
The distribution of energy such as translational and vibrational energies between the atoms and molecules in a system is important to whether a reaction trajectory is reactive or not. If in the system there is little kinetic or vibrational energy, the atom cannot cross the transition state because it does not have enough energy. Once the system has enough energy, the distribution between translational, vibrational and potential energy is important. After a system have enough energy to overcome the activation energy barrier, the excess energy the system possess will allow the middle atom to bounce back and force between the first and the third atom. Whether the second atom will stay with the first or the third atom depends on how much excess energy it has and therefore determines whether a new bond will form or not. As the excess energy increases incrementally, whether the reaction trajectory is reactive or not alternates. As shown in the exercise, an F atom and a H2 molecule approaching each other with little translational energy but enough energy above the activation energy barrier can lead to the formation of the product. There is almost no vibrational energy, once the H2 atom is pulled towards the F1 atom, it stick with it and does not bounce back.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system 5 7 reactive contour plot.png|thumb|center|400px|The contour plot of the F + H2 system when p1 = - 1.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2 = - 5.7 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is a reactive trajectory. Whether a reaction trajectory is reactive or not changes constantly for momenta p2 around -6.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system 5 6 unreactive contour plot.png|thumb|center|400px|The contour plot of the F + H2 system when p1 = - 1.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p2 = - 5.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is a unreactive trajectory. ]]&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_F_H_H_system_5_6_unreactive_contour_plot.png&amp;diff=805943</id>
		<title>File:YZ32918 F H H system 5 6 unreactive contour plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_F_H_H_system_5_6_unreactive_contour_plot.png&amp;diff=805943"/>
		<updated>2020-05-15T22:23:39Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805942</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805942"/>
		<updated>2020-05-15T22:23:24Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) kJ mol^{-1} = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H F F system activation energy surface plot 1.png|thumb|center|400px|The surface plot of how the energy of the transition state of the H + H-F reaction goes back to the energy of the reactant calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system energy vs time plot 1.png|thumb|center|400px|The energy vs time plot of the H + H-F reaction going from the transition state to the reactant.]]&lt;br /&gt;
&lt;br /&gt;
=== Release of the reaction energy ===&lt;br /&gt;
&lt;br /&gt;
The total energy of the reaction is conserved, when the F atom and a H2 molecule collided with each other, the H2 atom will bounce back and forth between the F1 atom and the H3 atom, whether the reaction trajectory is reactive or not depends on how much the initial kinetic energy of the F atom and H2 molecule have and how far the H3 atom is bumping away from F1 and H2. Initially, the system composed of F1 atom and H2 molecule, there will be no change of dipole moment when the H2 molecule vibrates and is IR inactive. If the reaction path is reactive, the product will be a H atom and a H-F molecule. If the H-F molecule vibrates, there will be a change in dipole moment and therefore IR active. We could observe a band due to the transition from v0 to v1 vibrational state and 1st and 2nd overtunes of the vibration. So the release of reaction energy can be measured by IR spectroscopy. Also, when a molecule vibrates, it radiates energy in the range of IR and the radiation can be detected. Also, calorimetry can be used to monitor the reaction as the reaction is exothermic and temperature will increase. If the reaction trajectory is not reactive, the reactant will remain the same so it will not be IR reactive.&lt;br /&gt;
&lt;br /&gt;
==== Reactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system reactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of a reactive trajectory of the F + H2 system. The orange line represents the vibration of the H2 molecule at the start which is not IR active and th blue line represents the vibration of the H-F molecule formed, there is a change in dipole moment, it is IR active.]]&lt;br /&gt;
&lt;br /&gt;
==== Unreactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system unreactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of an unreactive trajectory. The orange line represents the vibration of the H2 molecule, there is no change in dipole moment, so it is not IR active. The product is not formed and the reaction stays the same. The product is still IR inactive.]]&lt;br /&gt;
&lt;br /&gt;
=== Distribution of energy, position of transition state ===&lt;br /&gt;
&lt;br /&gt;
The distribution of energy such as translational and vibrational energies between the atoms and molecules in a system is important to whether a reaction trajectory is reactive or not. If in the system there is little kinetic or vibrational energy, the atom cannot cross the transition state because it does not have enough energy. Once the system has enough energy, the distribution between translational, vibrational and potential energy is important. After a system have enough energy to overcome the activation energy barrier, the excess energy the system possess will allow the middle atom to bounce back and force between the first and the third atom. Whether the second atom will stay with the first or the third atom depends on how much excess energy it has and therefore determines whether a new bond will form or not. As the excess energy increases incrementally, whether the reaction trajectory is reactive or not alternates. As shown in the exercise, an F atom and a H2 molecule approaching each other with little translational energy but enough energy above the activation energy barrier can lead to the formation of the product. There is almost no vibrational energy, once the H2 atom is pulled towards the F1 atom, it stick with it and does not bounce back.&lt;br /&gt;
&lt;br /&gt;
YZ32918 F H H system 5 7 reactive contour plot.png&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_F_H_H_system_5_7_reactive_contour_plot.png&amp;diff=805940</id>
		<title>File:YZ32918 F H H system 5 7 reactive contour plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_F_H_H_system_5_7_reactive_contour_plot.png&amp;diff=805940"/>
		<updated>2020-05-15T22:22:58Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805938</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805938"/>
		<updated>2020-05-15T22:22:42Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) kJ mol^{-1} = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H F F system activation energy surface plot 1.png|thumb|center|400px|The surface plot of how the energy of the transition state of the H + H-F reaction goes back to the energy of the reactant calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system energy vs time plot 1.png|thumb|center|400px|The energy vs time plot of the H + H-F reaction going from the transition state to the reactant.]]&lt;br /&gt;
&lt;br /&gt;
=== Release of the reaction energy ===&lt;br /&gt;
&lt;br /&gt;
The total energy of the reaction is conserved, when the F atom and a H2 molecule collided with each other, the H2 atom will bounce back and forth between the F1 atom and the H3 atom, whether the reaction trajectory is reactive or not depends on how much the initial kinetic energy of the F atom and H2 molecule have and how far the H3 atom is bumping away from F1 and H2. Initially, the system composed of F1 atom and H2 molecule, there will be no change of dipole moment when the H2 molecule vibrates and is IR inactive. If the reaction path is reactive, the product will be a H atom and a H-F molecule. If the H-F molecule vibrates, there will be a change in dipole moment and therefore IR active. We could observe a band due to the transition from v0 to v1 vibrational state and 1st and 2nd overtunes of the vibration. So the release of reaction energy can be measured by IR spectroscopy. Also, when a molecule vibrates, it radiates energy in the range of IR and the radiation can be detected. Also, calorimetry can be used to monitor the reaction as the reaction is exothermic and temperature will increase. If the reaction trajectory is not reactive, the reactant will remain the same so it will not be IR reactive.&lt;br /&gt;
&lt;br /&gt;
==== Reactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system reactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of a reactive trajectory of the F + H2 system. The orange line represents the vibration of the H2 molecule at the start which is not IR active and th blue line represents the vibration of the H-F molecule formed, there is a change in dipole moment, it is IR active.]]&lt;br /&gt;
&lt;br /&gt;
==== Unreactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system unreactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of an unreactive trajectory. The orange line represents the vibration of the H2 molecule, there is no change in dipole moment, so it is not IR active. The product is not formed and the reaction stays the same. The product is still IR inactive.]]&lt;br /&gt;
&lt;br /&gt;
=== Distribution of energy, position of transition state ===&lt;br /&gt;
&lt;br /&gt;
The distribution of energy such as translational and vibrational energies between the atoms and molecules in a system is important to whether a reaction trajectory is reactive or not. If in the system there is little kinetic or vibrational energy, the atom cannot cross the transition state because it does not have enough energy. Once the system has enough energy, the distribution between translational, vibrational and potential energy is important. After a system have enough energy to overcome the activation energy barrier, the excess energy the system possess will allow the middle atom to bounce back and force between the first and the third atom. Whether the second atom will stay with the first or the third atom depends on how much excess energy it has and therefore determines whether a new bond will form or not. As the excess energy increases incrementally, whether the reaction trajectory is reactive or not alternates. As shown in the exercise, an F atom and a H2 molecule approaching each other with little translational energy but enough energy above the activation energy barrier can lead to the formation of the product. There is almost no vibrational energy, once the H2 atom is pulled towards the F1 atom, it stick with it and does not bounce back.&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805806</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805806"/>
		<updated>2020-05-15T21:34:11Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) kJ mol^{-1} = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H F F system activation energy surface plot 1.png|thumb|center|400px|The surface plot of how the energy of the transition state of the H + H-F reaction goes back to the energy of the reactant calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system energy vs time plot 1.png|thumb|center|400px|The energy vs time plot of the H + H-F reaction going from the transition state to the reactant.]]&lt;br /&gt;
&lt;br /&gt;
=== Release of the reaction energy ===&lt;br /&gt;
&lt;br /&gt;
The total energy of the reaction is conserved, when the F atom and a H2 molecule collided with each other, the H2 atom will bounce back and forth between the F1 atom and the H3 atom, whether the reaction trajectory is reactive or not depends on how much the initial kinetic energy of the F atom and H2 molecule have and how far the H3 atom is bumping away from F1 and H2. Initially, the system composed of F1 atom and H2 molecule, there will be no change of dipole moment when the H2 molecule vibrates and is IR inactive. If the reaction path is reactive, the product will be a H atom and a H-F molecule. If the H-F molecule vibrates, there will be a change in dipole moment and therefore IR active. We could observe a band due to the transition from v0 to v1 vibrational state and 1st and 2nd overtunes of the vibration. So the release of reaction energy can be measured by IR spectroscopy. Also, when a molecule vibrates, it radiates energy in the range of IR and the radiation can be detected. Also, calorimetry can be used to monitor the reaction as the reaction is exothermic and temperature will increase. If the reaction trajectory is not reactive, the reactant will remain the same so it will not be IR reactive.&lt;br /&gt;
&lt;br /&gt;
==== Reactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system reactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of a reactive trajectory of the F + H2 system. The orange line represents the vibration of the H2 molecule at the start which is not IR active and th blue line represents the vibration of the H-F molecule formed, there is a change in dipole moment, it is IR active.]]&lt;br /&gt;
&lt;br /&gt;
==== Unreactive trajectory ====&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system unreactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of an unreactive trajectory. The orange line represents the vibration of the H2 molecule, there is no change in dipole moment, so it is not IR active. The product is not formed and the reaction stays the same. The product is still IR inactive.]]&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_F_H_H_system_unreactive_momenta_vs_time_plot.png&amp;diff=805786</id>
		<title>File:YZ32918 F H H system unreactive momenta vs time plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_F_H_H_system_unreactive_momenta_vs_time_plot.png&amp;diff=805786"/>
		<updated>2020-05-15T21:29:30Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805782</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805782"/>
		<updated>2020-05-15T21:28:54Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) kJ mol^{-1} = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H F F system activation energy surface plot 1.png|thumb|center|400px|The surface plot of how the energy of the transition state of the H + H-F reaction goes back to the energy of the reactant calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system energy vs time plot 1.png|thumb|center|400px|The energy vs time plot of the H + H-F reaction going from the transition state to the reactant.]]&lt;br /&gt;
&lt;br /&gt;
=== Release of the reaction energy ===&lt;br /&gt;
&lt;br /&gt;
The total energy of the reaction is conserved, when the F atom and a H2 molecule collided with each other, the H2 atom will bounce back and forth between the F1 atom and the H3 atom, whether the reaction trajectory is reactive or not depends on how much the initial kinetic energy of the F atom and H2 molecule have and how far the H3 atom is bumping away from F1 and H2. Initially, the system composed of F1 atom and H2 molecule, there will be no change of dipole moment when the H2 molecule vibrates and is IR inactive. If the reaction path is reactive, the product will be a H atom and a H-F molecule. If the H-F molecule vibrates, there will be a change in dipole moment and therefore IR active. We could observe a band due to the transition from v0 to v1 vibrational state and 1st and 2nd overtunes of the vibration. So the release of reaction energy can be measured by IR spectroscopy. Also, when a molecule vibrates, it radiates energy in the range of IR and the radiation can be detected. Also, calorimetry can be used to monitor the reaction as the reaction is exothermic and temperature will increase. If the reaction trajectory is not reactive, the reactant will remain the same so it will not be IR reactive.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system reactive momenta vs time plot.png|thumb|center|400px|The momenta vs time plot of a reactive trajectory of the F + H2 system. The orange line represents the vibration of the H2 molecule at the start which is not IR active and th blue line represents the vibration of the H-F molecule formed, there is a change in dipole moment, it is IR active.]]&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_F_H_H_system_reactive_momenta_vs_time_plot.png&amp;diff=805756</id>
		<title>File:YZ32918 F H H system reactive momenta vs time plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_F_H_H_system_reactive_momenta_vs_time_plot.png&amp;diff=805756"/>
		<updated>2020-05-15T21:20:18Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805753</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805753"/>
		<updated>2020-05-15T21:19:47Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) kJ mol^{-1} = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H F F system activation energy surface plot 1.png|thumb|center|400px|The surface plot of how the energy of the transition state of the H + H-F reaction goes back to the energy of the reactant calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system energy vs time plot 1.png|thumb|center|400px|The energy vs time plot of the H + H-F reaction going from the transition state to the reactant.]]&lt;br /&gt;
&lt;br /&gt;
=== Release of the reaction energy ===&lt;br /&gt;
&lt;br /&gt;
The total energy of the reaction is conserved, when the F atom and a H2 molecule collided with each other, the H2 atom will bounce back and forth between the F1 atom and the H3 atom, whether the reaction trajectory is reactive or not depends on how much the initial kinetic energy of the F atom and H2 molecule have and how far the H3 atom is bumping away from F1 and H2. Initially, the system composed of F1 atom and H2 molecule, there will be no change of dipole moment when the H2 molecule vibrates and is IR inactive. If the reaction path is reactive, the product will be a H atom and a H-F molecule. If the H-F molecule vibrates, there will be a change in dipole moment and therefore IR active. We could observe a band due to the transition from v0 to v1 vibrational state and 1st and 2nd overtunes of the vibration. So the release of reaction energy can be measured by IR spectroscopy. Also, when a molecule vibrates, it radiates energy in the range of IR and the radiation can be detected. Also, calorimetry can be used to monitor the reaction as the reaction is exothermic and temperature will increase. If the reaction trajectory is not reactive, the reactant will remain the same so it will not be IR reactive.&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805612</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805612"/>
		<updated>2020-05-15T20:40:26Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) kJ mol^{-1} = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H F F system activation energy surface plot 1.png|thumb|center|400px|The surface plot of how the energy of the transition state of the H + H-F reaction goes back to the energy of the reactant calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system energy vs time plot 1.png|thumb|center|400px|The energy vs time plot of the H + H-F reaction going from the transition state to the reactant.]]&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805253</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805253"/>
		<updated>2020-05-15T18:41:59Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H F F system activation energy surface plot 1.png|thumb|center|400px|The surface plot of how the energy of the transition state of the H + H-F reaction goes back to the energy of the reactant calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system energy vs time plot 1.png|thumb|center|400px|The energy vs time plot of the H + H-F reaction going from the transition state to the reactant.]]&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_H_F_F_system_activation_energy_surface_plot_1.png&amp;diff=805231</id>
		<title>File:YZ32918 H F F system activation energy surface plot 1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_H_F_F_system_activation_energy_surface_plot_1.png&amp;diff=805231"/>
		<updated>2020-05-15T18:34:27Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805227</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805227"/>
		<updated>2020-05-15T18:33:59Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
YZ32918 H H F system energy vs time plot 1.png&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_H_H_F_system_energy_vs_time_plot_1.png&amp;diff=805223</id>
		<title>File:YZ32918 H H F system energy vs time plot 1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_H_H_F_system_energy_vs_time_plot_1.png&amp;diff=805223"/>
		<updated>2020-05-15T18:33:24Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_H_H_F_system_energy_vs_time_plot.png&amp;diff=805210</id>
		<title>File:YZ32918 H H F system energy vs time plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_H_H_F_system_energy_vs_time_plot.png&amp;diff=805210"/>
		<updated>2020-05-15T18:29:00Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805206</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805206"/>
		<updated>2020-05-15T18:28:15Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Activation energy ====&lt;br /&gt;
&lt;br /&gt;
The activation energy is the energy difference between the transition state of a reaction and the energy of the reactant which is not kinetic. &lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = + 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;br /&gt;
&lt;br /&gt;
This system is the reverse of the F-H-H system that a H atom collide with the H-F molecule, the H-F bond is broken and a new H-H bond is formed. From the potential energy surface plot of this reaction we can see that this reaction is endothermic and this shows H-H bond is weaker than the H-F bond. According to the Hammond&#039;s postulate, the transition state will resemble the structure of the product and so the distance between H1-H2 is small and the distance between H2 and F3 is large.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 H H F system potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the H + H-F system, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the system is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found when the reactant is slightly displaced from the transition state and let it go back to the starting position and calculated using MEP. &lt;br /&gt;
&lt;br /&gt;
The activation energy is calculated as: &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.941 - (- 560.591) = + 126.650 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_H_H_F_system_potential_energy_surface_plot.png&amp;diff=805096</id>
		<title>File:YZ32918 H H F system potential energy surface plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_H_H_F_system_potential_energy_surface_plot.png&amp;diff=805096"/>
		<updated>2020-05-15T17:50:59Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805094</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805094"/>
		<updated>2020-05-15T17:50:43Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;br /&gt;
&lt;br /&gt;
=== H-H-F system ===&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805032</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805032"/>
		<updated>2020-05-15T17:29:58Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F H H system energy vs time plot.png|thumb|center|400px|Energy vs time plot of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system when setting the reactants at the transition state and calculated using MEP to obtain activation energy.]]&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_F_H_H_system_energy_vs_time_plot.png&amp;diff=805025</id>
		<title>File:YZ32918 F H H system energy vs time plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_F_H_H_system_energy_vs_time_plot.png&amp;diff=805025"/>
		<updated>2020-05-15T17:26:38Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805006</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=805006"/>
		<updated>2020-05-15T17:19:47Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The activation energy of the reaction is found by setting the system near the transition state at &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt; and let the system to go back to the reactants and then find the total energy of the system. Kinetic energy = 0, all the energy are potential energy. &lt;br /&gt;
&lt;br /&gt;
Activation energy = &amp;lt;math&amp;gt; {E_{TS}} - {E_{reactant}} = - 433.942 - (- 434.835) = 0.893 kJ mol^{-1} &amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=804318</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=804318"/>
		<updated>2020-05-15T12:57:48Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;br /&gt;
&lt;br /&gt;
The transition state of the reaction is found to be approximately: &amp;lt;math&amp;gt; {r_{FH}} = 181.390 pm, {r_{HH}} = 74 pm&amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=804286</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=804286"/>
		<updated>2020-05-15T12:48:16Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 F+H2 potential energy surface plot.png|thumb|center|400px|The potential energy surface plot of the F+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the reactant is on the right-hand side and the product is on the left-hand side.]]&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_F%2BH2_potential_energy_surface_plot.png&amp;diff=804281</id>
		<title>File:YZ32918 F+H2 potential energy surface plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_F%2BH2_potential_energy_surface_plot.png&amp;diff=804281"/>
		<updated>2020-05-15T12:45:11Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=804280</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=804280"/>
		<updated>2020-05-15T12:44:40Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== F-H-H system ===&lt;br /&gt;
&lt;br /&gt;
The F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic as can be seen from the potential energy surface. The H-H bond is broken and a new H-F bond is formed during the reaction. This sugguests the H-F bond is stronger than the H-H bond. According to Hammond&#039;s postulate, the structure of the transition state will resemble the structure of reactant or product that is closer in energy. So, the transition state of the reaction will be similar to the reactant when H2-H3 distance is small and F1-H2 distance is large. The transition state is early and it will be relocated closer to the reactant.&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=804011</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=804011"/>
		<updated>2020-05-15T10:43:34Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;br /&gt;
&lt;br /&gt;
=== H-F-H system ===&lt;br /&gt;
&lt;br /&gt;
The H-F-H system is a symmetric molecule, the reactant and the product are the same, therefore, the transition state is also symmetric. There will be no force acting along AB or BC. The distance between H-F is found to be: &amp;lt;math&amp;gt; {r_{HF}} = 103.817 pm&amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803723</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803723"/>
		<updated>2020-05-14T22:10:58Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;br /&gt;
&lt;br /&gt;
==== Transition State Theory ====&lt;br /&gt;
&lt;br /&gt;
The Transition State Theory will overestimate the rate of reaction compared to experimental values because an important assumption in the Transition State Theory is all the trajectories along the reaction coordinate with kinetic energy greater than the activation energy will be reactive. But we have seen in the above examples that this is not the case and they are not all reactive.&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803710</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803710"/>
		<updated>2020-05-14T22:03:58Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
From the conditions shown above, we can see that whether a reaction path is reactive or not does not necessarily depends on whether the molecules have enough energy to cross the transition state but importantly, it depends on the kinetic energy distribution between the products, their velocities and momentum. Even if the total energy of a system is large enough, the reaction may still not be reactive.&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803694</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803694"/>
		<updated>2020-05-14T21:49:32Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 5 contour plot.png|300px]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_reaction_trajectory_table_5_contour_plot.png&amp;diff=803693</id>
		<title>File:YZ32918 reaction trajectory table 5 contour plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_reaction_trajectory_table_5_contour_plot.png&amp;diff=803693"/>
		<updated>2020-05-14T21:49:03Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803691</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803691"/>
		<updated>2020-05-14T21:48:49Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 4 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_reaction_trajectory_table_4_contour_plot.png&amp;diff=803689</id>
		<title>File:YZ32918 reaction trajectory table 4 contour plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_reaction_trajectory_table_4_contour_plot.png&amp;diff=803689"/>
		<updated>2020-05-14T21:48:21Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803688</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803688"/>
		<updated>2020-05-14T21:48:06Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 3 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_reaction_trajectory_table_3_contour_plot.png&amp;diff=803687</id>
		<title>File:YZ32918 reaction trajectory table 3 contour plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_reaction_trajectory_table_3_contour_plot.png&amp;diff=803687"/>
		<updated>2020-05-14T21:47:33Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803685</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803685"/>
		<updated>2020-05-14T21:47:10Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. || [[File:YZ32918 reaction trajectory table 2 contour plot.png|300px]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_reaction_trajectory_table_2_contour_plot.png&amp;diff=803684</id>
		<title>File:YZ32918 reaction trajectory table 2 contour plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_reaction_trajectory_table_2_contour_plot.png&amp;diff=803684"/>
		<updated>2020-05-14T21:45:57Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803682</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803682"/>
		<updated>2020-05-14T21:45:23Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || - 420.077 || Unreactive || H3 atom collided with H1-H2 molecule and bounced back ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || - 413.977 || Reactive || H3 atom collided with H1-H2 molecule and has just the enough energy to form a new bond and travel away with significant vibrational energy ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 || Unreactive || H3 atom collided with H1-H2 molecule and formed a new bond for a very short time but vibrates vigorously, the new bond is broken and H3 is bounced back. ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || - 349.477 || Reactive || H3 atom collided with H1-H2 molecule, pulled the H2 atom away from H1 atom, the H2 atom bounced back with H1 atom and then bounced back towards H3 atom to form new H2-H3 bond and H1 atom. ||&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803653</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803653"/>
		<updated>2020-05-14T21:17:04Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|300px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || || || ||&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803649</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803649"/>
		<updated>2020-05-14T21:16:00Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|200px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || || || ||&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803648</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803648"/>
		<updated>2020-05-14T21:15:38Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png|150px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || || || ||&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803647</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803647"/>
		<updated>2020-05-14T21:15:07Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 || [[File:YZ32918 reaction trajectory table 1 contour plot.png]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || || || ||&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_reaction_trajectory_table_1_contour_plot.png&amp;diff=803645</id>
		<title>File:YZ32918 reaction trajectory table 1 contour plot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:YZ32918_reaction_trajectory_table_1_contour_plot.png&amp;diff=803645"/>
		<updated>2020-05-14T21:13:51Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803644</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803644"/>
		<updated>2020-05-14T21:13:27Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || - 414.280 || Reactive || H3 collided with H1-H2 to generate H1 and H2-H3 ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || || || ||&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803635</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803635"/>
		<updated>2020-05-14T21:05:38Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;br /&gt;
&lt;br /&gt;
==== Reactive and unreactive paths ====&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || || || ||&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803590</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803590"/>
		<updated>2020-05-14T20:35:21Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803589</id>
		<title>MRD:oirewajgoijreoij234502850437603284</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:oirewajgoijreoij234502850437603284&amp;diff=803589"/>
		<updated>2020-05-14T20:33:20Z</updated>

		<summary type="html">&lt;p&gt;Yz32918: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Transition State ==&lt;br /&gt;
&lt;br /&gt;
=== Explanation ===&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface, a transition state is a stationary point:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { \partial F(x,y)\over \partial x} = 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; { \partial F(x,y)\over \partial y} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and further: &amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;lt; 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be identified as a maximum in along the bond direction and minimum in the direction orthogonal to the bond. The transition state is different from a local energy minimum, the local energy minimum is given by the condition:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; { {\partial^2 F(x,y)\over \partial x^2} {\partial^2 F(x,y)\over \partial y^2}-({\partial^2 F(x,y)\over \partial x y})^2} &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; { \partial^2 F(x,y)\over \partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state Surface Plot 3.png|thumb|center|400px|Illustration of the transition state]]&lt;br /&gt;
&lt;br /&gt;
A local minimum on the potential energy surface can be distinguished because all the points around it will have larger values but for a saddle point some point will have larger values and others have smaller values.&lt;br /&gt;
&lt;br /&gt;
==== Transition state position ====&lt;br /&gt;
&lt;br /&gt;
The estimate for the transition state position is &amp;lt;math&amp;gt; {r_{ts}} = 90.777 pm&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt; {r_{AB}} = {r_{BC}} = 90.777 pm&amp;lt;/math&amp;gt;. This is a position where there is no force acting along AB or BC, the atoms A, B, C are stationary, there is no kinetic energy and only potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 transition state position internuclear distance vs time plot.png|thumb|center|400px|Internuclear distance vs time plot for transition state position]]&lt;br /&gt;
&lt;br /&gt;
==== Reaction path trajectories ====&lt;br /&gt;
&lt;br /&gt;
In minimum energy path (mep) calculations, the hydrogen atoms in the molecule formed does not vibration as they move away, the reaction path is a straight line. In Dynamics calculations, the molecule vibrates as it move away, the reaction path is wiggling.&lt;br /&gt;
&lt;br /&gt;
[[File:YZ32918 reaction path MEP contour plot.png|thumb|center|400px|Reaction path calculated using MEP.]]&lt;br /&gt;
[[File:YZ32918 reation path Dynamics contour plot.png|thumb|center|400px|Reaction path calculated using Dynamics.]]&lt;/div&gt;</summary>
		<author><name>Yz32918</name></author>
	</entry>
</feed>