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	<id>https://chemwiki.ch.ic.ac.uk/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=Pp4717</id>
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	<updated>2026-05-28T13:24:20Z</updated>
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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=782978</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=782978"/>
		<updated>2019-05-17T12:07:11Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
===On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?===&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:Ts01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; For the H + HF reaction: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:TSIND01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.802 Â&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction:&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; For the H + HF reaction: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:TS201333428.png]]&lt;br /&gt;
&lt;br /&gt;
Activation energy = 0.009 KCal/mol&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.===&lt;br /&gt;
&lt;br /&gt;
[[File:Initialconditions01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
These set of initial conditions give the reactive trajectory for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780937</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780937"/>
		<updated>2019-05-16T14:35:03Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
===On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?===&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:Ts01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; For the H + HF reaction: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:TSIND01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.802 Â&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction:&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; For the H + HF reaction: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:TS201333428.png]]&lt;br /&gt;
&lt;br /&gt;
Activation energy = 0.009 KCal/mol&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.===&lt;br /&gt;
&lt;br /&gt;
[[File:Initialconditions01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
These set of initial conditions give the reactive trajectory for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780933</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780933"/>
		<updated>2019-05-16T14:34:21Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
===On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?===&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction: &amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:Ts01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; For the H + HF reaction: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:TSIND01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.802 Â&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction:&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; For the H + HF reaction: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:TS201333428.png]]&lt;br /&gt;
&lt;br /&gt;
Activation energy = 0.009 KCal/mol&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.===&lt;br /&gt;
&lt;br /&gt;
[[File:Initialconditions01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
These set of initial conditions give the reactive trajectory for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780917</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780917"/>
		<updated>2019-05-16T14:31:50Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Ts01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
For the H + HF reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:TSIND01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.802 Â&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;br /&gt;
&lt;br /&gt;
For the H + HF reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:TS201333428.png]]&lt;br /&gt;
&lt;br /&gt;
Activation energy = 0.009 KCal/mol&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.===&lt;br /&gt;
&lt;br /&gt;
[[File:Initialconditions01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
These set of initial conditions give the reactive trajectory for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780912</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780912"/>
		<updated>2019-05-16T14:30:40Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
[[File:TS pp01333427.PNG]]&lt;br /&gt;
&lt;br /&gt;
[[File:Ts01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
For the H + HF reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:TSIND01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.802 Â&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;br /&gt;
&lt;br /&gt;
For the H + HF reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:TS201333428.png]]&lt;br /&gt;
&lt;br /&gt;
Activation energy = 0.009 KCal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:TSIND01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.802 Â&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.===&lt;br /&gt;
&lt;br /&gt;
[[File:Initialconditions01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
These set of initial conditions give the reactive trajectory for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780886</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780886"/>
		<updated>2019-05-16T14:26:02Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:TS pp01333427.PNG]]&lt;br /&gt;
&lt;br /&gt;
[[File:Ts01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;br /&gt;
&lt;br /&gt;
For the H + HF reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:TSIND01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.802 Â&lt;br /&gt;
&lt;br /&gt;
[[File:TS201333428.png]]&lt;br /&gt;
&lt;br /&gt;
Activation energy = 0.009 KCal/mol&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.===&lt;br /&gt;
&lt;br /&gt;
[[File:Initialconditions01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
These set of initial conditions give the reactive trajectory for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Initialconditions01333428.PNG&amp;diff=780870</id>
		<title>File:Initialconditions01333428.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Initialconditions01333428.PNG&amp;diff=780870"/>
		<updated>2019-05-16T14:24:12Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780724</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780724"/>
		<updated>2019-05-16T14:06:45Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:TS pp01333427.PNG]]&lt;br /&gt;
&lt;br /&gt;
[[File:Ts01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;br /&gt;
&lt;br /&gt;
For the H + HF reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:TSIND01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.802 Â&lt;br /&gt;
&lt;br /&gt;
[[File:TS201333428.png]]&lt;br /&gt;
&lt;br /&gt;
Activation energy = 0.009 KCal/mol&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.===&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780698</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780698"/>
		<updated>2019-05-16T14:03:50Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:TS pp01333427.PNG]]&lt;br /&gt;
&lt;br /&gt;
[[File:Ts01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;br /&gt;
&lt;br /&gt;
For the H + HF reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:TSIND01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.802 Â&lt;br /&gt;
&lt;br /&gt;
[[File:TS201333428.png]]&lt;br /&gt;
&lt;br /&gt;
Activation energy = 0.009 KCal/mol&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.=&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780695</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780695"/>
		<updated>2019-05-16T14:03:28Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:TS pp01333427.PNG]]&lt;br /&gt;
&lt;br /&gt;
[[File:Ts01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;br /&gt;
&lt;br /&gt;
For the H + HF reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:TSIND01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.802 Â&lt;br /&gt;
&lt;br /&gt;
[[File:TS201333428.png]]&lt;br /&gt;
&lt;br /&gt;
Activation energy = 0.009 KCal/mol&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.==&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780689</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780689"/>
		<updated>2019-05-16T14:02:30Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:TS pp01333427.PNG]]&lt;br /&gt;
&lt;br /&gt;
[[File:Ts01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;br /&gt;
&lt;br /&gt;
For the H + HF reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:TSIND01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.802 Â&lt;br /&gt;
&lt;br /&gt;
[[File:TS201333428.png]]&lt;br /&gt;
&lt;br /&gt;
Activation energy = 0.009 KCal/mol&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:TSIND01333428.png&amp;diff=780674</id>
		<title>File:TSIND01333428.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:TSIND01333428.png&amp;diff=780674"/>
		<updated>2019-05-16T14:00:25Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780663</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780663"/>
		<updated>2019-05-16T13:59:26Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:TS pp01333427.PNG]]&lt;br /&gt;
&lt;br /&gt;
[[File:Ts01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
For the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;br /&gt;
&lt;br /&gt;
For the H + HF reaction:&lt;br /&gt;
&lt;br /&gt;
[[File:TS201333428.png]]&lt;br /&gt;
&lt;br /&gt;
Activation energy = 0.009 KCal/mol&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:TS201333428.png&amp;diff=780645</id>
		<title>File:TS201333428.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:TS201333428.png&amp;diff=780645"/>
		<updated>2019-05-16T13:57:27Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780387</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780387"/>
		<updated>2019-05-16T13:29:29Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:TS pp01333427.PNG]]&lt;br /&gt;
&lt;br /&gt;
[[File:Ts01333428.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Ts01333428.PNG&amp;diff=780379</id>
		<title>File:Ts01333428.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Ts01333428.PNG&amp;diff=780379"/>
		<updated>2019-05-16T13:28:44Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780357</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780357"/>
		<updated>2019-05-16T13:25:34Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:TS pp01333427.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;br /&gt;
&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction = 29.474 KCal/mol&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780288</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780288"/>
		<updated>2019-05-16T13:15:35Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:TS pp01333427.PNG]]&lt;br /&gt;
&lt;br /&gt;
The transition state is located at 1.83 Ǎ.&lt;br /&gt;
&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
[[File:ActivationenergyFHH pp01333428.png]]&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:ActivationenergyFHH_pp01333428.png&amp;diff=780280</id>
		<title>File:ActivationenergyFHH pp01333428.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:ActivationenergyFHH_pp01333428.png&amp;diff=780280"/>
		<updated>2019-05-16T13:14:31Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780259</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780259"/>
		<updated>2019-05-16T13:10:37Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;br /&gt;
&lt;br /&gt;
[[File:TS pp01333427.PNG]]&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:TS_pp01333427.PNG&amp;diff=780255</id>
		<title>File:TS pp01333427.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:TS_pp01333427.PNG&amp;diff=780255"/>
		<updated>2019-05-16T13:10:03Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Pp47175.png&amp;diff=780157</id>
		<title>File:Pp47175.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Pp47175.png&amp;diff=780157"/>
		<updated>2019-05-16T12:48:37Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Pp47174.png&amp;diff=780156</id>
		<title>File:Pp47174.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Pp47174.png&amp;diff=780156"/>
		<updated>2019-05-16T12:48:15Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Pp47173.png&amp;diff=780155</id>
		<title>File:Pp47173.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Pp47173.png&amp;diff=780155"/>
		<updated>2019-05-16T12:47:58Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Pp47172.png&amp;diff=780153</id>
		<title>File:Pp47172.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Pp47172.png&amp;diff=780153"/>
		<updated>2019-05-16T12:47:37Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780152</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780152"/>
		<updated>2019-05-16T12:47:11Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|[[File:pp47172.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47173.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|[[File:pp47174.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|[[File:pp47175.png]]&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780147</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780147"/>
		<updated>2019-05-16T12:45:44Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.png]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Pp47171.png&amp;diff=780146</id>
		<title>File:Pp47171.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Pp47171.png&amp;diff=780146"/>
		<updated>2019-05-16T12:45:28Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: Pp4717 uploaded a new version of File:Pp47171.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780132</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=780132"/>
		<updated>2019-05-16T12:42:21Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|[[File:pp47171.PNG]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=778777</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=778777"/>
		<updated>2019-05-14T19:51:57Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is generated from making a skew plot to form coordinates q1 and q2. The coordinates q1 and q2 are then differentiated and the minimum of one curve is the maximum of the other. The point at which the minimum and maximum converge is the transition state. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
F +  H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is an exothermic reaction; this shows that the bond strength is strong.&lt;br /&gt;
&lt;br /&gt;
H + HF is endothermic; this shows that the bond strength is weak.&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=CP3MD&amp;diff=778751</id>
		<title>CP3MD</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=CP3MD&amp;diff=778751"/>
		<updated>2019-05-14T19:10:25Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
&lt;br /&gt;
== The software ==&lt;br /&gt;
&lt;br /&gt;
Download the [https://github.com/imperialchem/mrd-demo/archive/master.zip zip archive] with the software and data files required for this experiment.&lt;br /&gt;
&lt;br /&gt;
Extract the content of the archive and run the &#039;&#039;lepsgui.py&#039;&#039; file to start the program. If this doesn&#039;t work you will need to run the program from the command line. To do this on Windows follow the steps:&lt;br /&gt;
&lt;br /&gt;
# Using the File Explorer navigate to the directory where the files are.&lt;br /&gt;
# On the File tab on the top of the window select &amp;quot;Open Windows PowerShell&amp;quot;.&lt;br /&gt;
# Type &#039;&#039;python lepsgui.py&#039;&#039; to run the program.&lt;br /&gt;
&lt;br /&gt;
(If the last step fails, there might be an issue with your python installation and the python interpreter is not in your PATH. In that case you will need to type the full path of the &#039;&#039;python.exe&#039;&#039; file on your system.)&lt;br /&gt;
&lt;br /&gt;
== Introduction ==&lt;br /&gt;
&lt;br /&gt;
=== Objectives ===&lt;br /&gt;
&#039;&#039;&#039;The objectives of this exercise are to study the reactivity of triatomic systems, where an atom and a diatomic molecule collide, through calculating Molecular Dynamics trajectories.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
This exercise is designed to make you think about transition states, reaction coordinates and potential energy surfaces. You should discover that, for a chemical reaction to take place, having sufficient energy to overcome a barrier is not enough: the energy must also be in the right vibrational modes at the right time. You&#039;ll see trajectories cross the barrier, as if a reaction is going to take place, but then go back to reactants, with energy exchanged between translation and vibration.&lt;br /&gt;
&lt;br /&gt;
The gas phase collision and reaction between an atom and diatomic molecule in a linear configuration will be studied. If the reaction proceeds it will form a new diatomic molecule and atom. This exercise builds a level of sophistication upon previous kinetic treatments that you have seen by examining other types of energy (e.g. vibrational) that may be needed for reaction or present in products and also by illustrating how certain conditions lead to reaction profiles which simpler models do not predict.&lt;br /&gt;
&lt;br /&gt;
=== The write-up Required ===&lt;br /&gt;
In this lab you will be writing a report of your results in the form of a wiki. You should {{fontcolor1|blue|explicitly address questions highlighted in blue in the script}} and backup your answers with results and illustrations of calculations you perform using the program.&lt;br /&gt;
&lt;br /&gt;
To start your report choose a URL of the form &amp;lt;nowiki&amp;gt;https://wiki.ch.ic.ac.uk/wiki/index.php?title=&amp;lt;/nowiki&amp;gt;{{fontcolor1|black|yellow|MRD:anything}}, insert it on the address bar of the browser and start editing. The URL you choose must be unique. All figure files you upload to the wiki must also have unique names. A good way of generating unique URLs and files names is by adding your CID or college login to them. &#039;&#039;&#039;Do not ignore any wiki warnings about file name clashes.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Using the wiki visual editor should be sufficient to write your report. If you want to edit the source of your wiki some [[Title%3DMod:inorganic_wiki_page_instructions |general instructions]] are available, and you can also search the web.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;After some time without saving your work (about 30 min) the wiki system might log you out and you may lose unsaved changes. To avoid this, choose the &amp;quot;Keep me logged in&amp;quot; option when you login or save your work regularly.&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Submit the address of your wiki via Blackboard. Only edits completed before 18:00 on the Friday in the week you are scheduled to do the exercise will be considered.&lt;br /&gt;
&lt;br /&gt;
=== Relevance to other courses ===&lt;br /&gt;
&lt;br /&gt;
A lot of the background material for this exercise has been covered in courses you have taken during year 1 and 2.&lt;br /&gt;
&lt;br /&gt;
* Molecular Driving Forces (intermolecular interactions - Prof. Ian Gould)&lt;br /&gt;
* Chemical Kinetics (collision theory, Maxwell-Boltzmann distribution of velocities - Prof. Oscar Ces)&lt;br /&gt;
* Statistical Thermodynamics (Boltzmann distribution, translational and vibrational partition functions - Prof. Nick Quirke)&lt;br /&gt;
* Introduction to Physical Organic Chemistry  (Transition states, activation enthalpies, reaction energy profiles - Prof. Ian McCulloch).&lt;br /&gt;
&lt;br /&gt;
Having completed the exercise you will be better prepared to understand material in year 3 where the Molecular Reaction Dynamics course (Prof Yaliraki) in particular builds on the ideas and concepts developed here.&lt;br /&gt;
&lt;br /&gt;
=== Theory ===&lt;br /&gt;
&lt;br /&gt;
==== Introduction ====&lt;br /&gt;
&lt;br /&gt;
It is possible to simulate a chemical reaction by describing the relative motion of the atoms that occurs while the reaction takes place. Since the mass of the atoms is relatively large (compare with the mass of the electron for example), for many chemical reactions it is possible to assume that the motion of the atoms follow Newton&#039;s equations of motion, i.e. obey classical mechanics. This is an approximation, since it neglects the fact that molecular vibrations are quantized or quantum tunneling effects, but it is nevertheless a good approximation for most chemical reactions.&lt;br /&gt;
&lt;br /&gt;
The relative motion of the atoms will depend on the interaction between them, which in turn depends on their relative position (for example, how far their nuclei are from each other). Interatomic interactions, as part of a molecule or not, are expressed as a &#039;&#039;&#039;potential energy surface&#039;&#039;&#039; &#039;&#039;&#039;V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;,...)&#039;&#039;&#039; which represent the potential energy of the system as a function of the atoms&#039; relative positions defined by the different internal coordinates &#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;. (For a diatomic molecule &#039;&#039;&#039;V(r) &#039;&#039;&#039;is just the usual [[#diatomic potential|potential energy curve]] that expresses the change in the energy as the two nuclei are displaced from their equilibrium positions by changing the interatomic distance – making the separation too small leads to a rapid rise in potential energy and increasing the bond length also leads to an increase in energy and eventually to dissociation).&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div id=&amp;quot;diatomic potential&amp;quot;&amp;gt;&lt;br /&gt;
[[File:Diatomic_Potential.svg|thumb|none|350px|Potential energy as a function of the interatomic distance for a diatomic molecule.]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The force (variation of momentum &#039;&#039;&#039;p&#039;&#039;&#039;) acting on a given interatomic coordinate &#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039; will depend on the derivative of the potential energy surface with respect to that coordinate.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; {dp_i \over dt} = - { \partial V(r_1,r_2,...)\over \partial r_i}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
By solving the equations of motion we are able to determine the trajectory of the system, i.e. determine the relative position of the atoms at each instant in time &#039;&#039;&#039;r&#039;&#039;&#039;(t). The trajectory represents a path across the potential energy surface (you will see examples shortly), and can be used to gain insight on how the reaction might proceed.&lt;br /&gt;
&lt;br /&gt;
Such simulations have many applications in chemistry and biology and you may well encounter these in higher level lecture courses in year 4.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Note that the program does all these calculations for you. You input bond distances and momenta for the atoms specified and the potential energy surface and the trajectory the system follows across the surface is calculated for you. Your job is to interpret the results.&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
==== Atom-Diatom Collisions ====&lt;br /&gt;
In this exercise we will apply this method to study atom diatom collisions. A typical example is depicted below.&lt;br /&gt;
&lt;br /&gt;
[[File:Y2C1.png|frameless|centre|400px]]&lt;br /&gt;
&lt;br /&gt;
In simple terms, the atom m&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; collides with the molecule and forms a new molecule with m&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, while m&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is detached as a separate atom. &lt;br /&gt;
&lt;br /&gt;
If we think about how the distances r&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; change during this process we can make several deductions. &lt;br /&gt;
&lt;br /&gt;
Before the collision/reaction:&lt;br /&gt;
* r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will be approximately constant (it will oscillate slightly if the molecule has vibrational energy).&lt;br /&gt;
* r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is decreasing steadily as m&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;gets closer to m&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
After the collision/reaction:&lt;br /&gt;
* r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; will now be approximately constant (but it will oscillate slightly if the molecule has vibrational energy).&lt;br /&gt;
* r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is increasing steadily as m&amp;lt;sub&amp;gt;3 &amp;lt;/sub&amp;gt;moves away from the molecule formed from m&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt; and m&amp;lt;sub&amp;gt;1.&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This means that instead of our simple picture of energy versus reaction coordinate we can map the progress of this reaction on a potential energy surface where potential energy is plotted as a function of both r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. A &#039;&#039;&#039;trajectory&#039;&#039;&#039; {&#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t)} can then be drawn on this potential energy surface. In a first instance, one can think of this trajectory in terms of that a sphere rolling of potential energy shaped surface would follow. However this analogy in the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; coordinates is not accurate, as the system is not really formed by a single rolling mass but several interacting masses. (As will be discussed further below, the rolling sphere analogy can be made accurate via a change of coordinates which distort the potential energy surfaces.)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div id=&amp;quot;triatomic surface&amp;quot;&amp;gt;&lt;br /&gt;
[[File:Y2C2.png|thumb|800px|none|An example of a reactive trajectory for an H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; type potential surface. The small boxes indicate the reactants (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; large &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; small), a transition structure where &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=&#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, &#039;&#039;&#039;and the products (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; small &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; large). (Note that the variation of potential energy along the combined r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; axes is the typical reaction profile curve you have seen before).]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The general triatomic system depicted means we started with atom A and molecule BC and ended with molecule AB and atom C. A &#039;&#039;reactive trajectory&#039;&#039; that passes through the &#039;&#039;&#039;transition structure&#039;&#039;&#039; is shown as a wavy line. The transition structure is a saddle point in the potential energy surface. Notice that the trajectory shown involves vibration in &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; (the molecule BC has vibrational energy) as the inter-fragment distance &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; is decreased in the &#039;&#039;entrance&#039;&#039; channel (at the top left of the figure) and vibration in &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; (the product AB has vibrational energy) as the inter-fragment distance &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; is increased in the &#039;&#039;exit&#039;&#039; channel (at the right of the figure). An &#039;&#039;unreactive trajectory&#039;&#039; would bounce off the barrier or its surroundings and regenerate the reactants.   &lt;br /&gt;
&lt;br /&gt;
For a given potential surface, the outcome of a dynamics simulation (i.e. the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t), &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t),&#039;&#039;&#039; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t)) at some time t are determined by the initial conditions at time t=0 (i.e. &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(0), &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(0) and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(0),&#039;&#039;&#039; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(0)). &lt;br /&gt;
&lt;br /&gt;
In the program you will use, you will run trajectories on different potential surfaces - corresponding to different triatomic chemical systems - for a variety of input conditions.  You will be able to animate the trajectory on the potential surface and examine the distribution of vibrational and translational energy in the products. &lt;br /&gt;
&lt;br /&gt;
You will first study the potential surface for an atom of H colliding with a molecule of hydrogen to illustrate the principles and to learn how to use the main features of the program. You will then move to look at other reaction examples.&lt;br /&gt;
&lt;br /&gt;
== EXERCISE 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system  ==&lt;br /&gt;
The first stages of this exercise are designed to develop your understanding of potential energy surfaces, reaction coordinates, transition structures, and to introduce the difference between kinetics and dynamics which can be studied experimentally. It is also meant to familiarise you with the main features of the program you will be using.&lt;br /&gt;
&lt;br /&gt;
=== Coordinates ===&lt;br /&gt;
&lt;br /&gt;
Before you begin experimenting with the different types of collision, note that the script makes reference to r&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; whereas in the GUI the atoms are currently labelled A B and C and the distances are r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. Since you run some trajectories in both forward and reverse directions it is hard to develop a consistent notation. Thus before you run a trajectory, check carefully what you have set up. Your initial molecule will be defined by which of the AB  or BC distances you have set to be the bond distance. One distance will be short (the bond distance) and one will be long. &lt;br /&gt;
&lt;br /&gt;
=== Running and visualising a trajectory ===&lt;br /&gt;
In this part you are given a set of conditions such that the reaction depicted below will proceed.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div id=&amp;quot;reactive conditions&amp;quot;&amp;gt;&lt;br /&gt;
[[File:Y2C5.png|frameless|500px|centre]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
We first set up the calculation of how the atoms position and momenta change with time, and then we will analyse the results of this calculation&lt;br /&gt;
&lt;br /&gt;
The program has a set of initial conditions and will run with those when you first run &#039;&#039;lepsgui.py&#039;&#039; and should show you a contour plot. &lt;br /&gt;
&lt;br /&gt;
* Change the initial condition in the settings window to run the example above: check the initial conditions that are shown in the menu agree with the figure (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(0) = 0.74  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(0) = 2.30  and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(0)=0 &#039;&#039;&#039; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(0) = -2.7).&lt;br /&gt;
&lt;br /&gt;
For &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0, a &#039;&#039;negative&#039;&#039; value of &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; corresponds to a &#039;&#039;decrease&#039;&#039; in the interatomic distance &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;.  By choosing these initial conditions, we are thus setting the system in motion in such a way as to initially decrease &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; (refer to the diagram above).&lt;br /&gt;
&lt;br /&gt;
In this case BC is the molecule with a bond distance = 0.74 and A is the atom that collides with it. Thus here r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
These initial conditions of the positions and momenta produce a &#039;&#039;reactive trajectory&#039;&#039; (like the [[#triatomic surface|example above]]). In other words, these conditions lead to the reaction taking place. As you will see in later sections, not all trajectories you run will be reactive.&lt;br /&gt;
&lt;br /&gt;
The program updates the image on the separate dedicated window when you press the “Update Plot” button at the bottom left of the settings window. By default the program will show you the trajectory corresponding to the input initial conditions and the contour plot of the Potential Energy Surface (PES). To see other plots, such as plots of positions and momenta against time, or a 3D surface plot of the reaction, select that option from the &amp;quot;Plot Type&amp;quot; menu at the centre of the interface and press &amp;quot;Update Plot&amp;quot;. Spend some time to have a look at the various options:&lt;br /&gt;
&lt;br /&gt;
* Selecting &amp;quot;Skew Plot&amp;quot; will produce a potential energy contour plot on a different set of coordinates Q&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and Q&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, where the oblique mesh defines the direction of the coordinates r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;. The new coordinates are defined as:&lt;br /&gt;
&amp;lt;math&amp;gt;\begin{align}&lt;br /&gt;
&amp;amp;Q_1=\sqrt{\mu_{A,BC}} \ r_{BC} + \sqrt{\mu_{C,AB}} \ r_{AB} \cos(\beta) \\&lt;br /&gt;
&amp;amp;Q_2=\sqrt{\mu_{C,AB}} \ r_{AB} \sin(\beta)&lt;br /&gt;
\end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\begin{align}&lt;br /&gt;
&amp;amp;\mu_{A,BC}=\frac{m_A (m_B+m_C)}{m_A+m_B+m_C}\\&lt;br /&gt;
&amp;amp;\mu_{C,AB}=\frac{m_C (m_A+m_B)}{m_A+m_B+m_C}\\&lt;br /&gt;
&amp;amp;\cos^2(\beta)=\frac{m_A m_C}{(m_A+m_B)(m_B+m_C)}&lt;br /&gt;
\end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where β is the so called Skew angle setting the angle of the oblique mesh. The advantage of this set of coordinates is that the dynamics of the system can be analysed as a rolling sphere on a potential surface, where the force acting on the trajectory is orthogonal to the contour lines. (If you are interested in the details, check the [[#bibliography|further reading]] section.)&lt;br /&gt;
&lt;br /&gt;
* Select “Surface Plot”, which gives you a plot of the PES in the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; coordinates. You can have a better look at the surface plot by rotating it with the mouse. Try to identify the reactant and product channels and the maximum potential energy along the valley floor. The trail of black dots along the bottom of the potential is the trajectory followed by the system. Observe how the trajectory is wavy: this indicates that the diatomic molecule is vibrating. An important point to observe is conservation of energy: the system will always oscillate between energy contours with the same value.&lt;br /&gt;
&lt;br /&gt;
* To animate the geometry, select the last option, “Animation”, in the &amp;quot;Plot Type&amp;quot; menu. You will see that initially r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; decreases as H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, then after the transition state, H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; leaves and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is formed in a vibrationally excited state.&lt;br /&gt;
&lt;br /&gt;
* This same information can be displayed in a different form by selecting “Internuclear Distances vs Time” in the same menu. In this graphical display the values of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;(t), r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(t) are given (Y axis) against time t (X axis). Notice that r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; here) decreases from the original value of 2.3 during the first 0.38 time units, then it has an oscillatory behaviour for the remainder of the trajectory corresponding to H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; vibration.  In contrast r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; here) has a slight oscillatory behaviour initially, then after the transition state, it grows in value as H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; leaves. Notice that r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;(t) = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(t) at ≈ 0.38 time units, and in this case is quite close to the transition state structure (this is not the case for all trajectories).&lt;br /&gt;
&lt;br /&gt;
[[File:Y2C7.png|thumb|800px|none|r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;(t) and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(t) are given (Y axis) against time t (X axis). Note that only two distances are shown on this plot. The GUI shows three.]]&lt;br /&gt;
&lt;br /&gt;
* The &amp;quot;Internuclear velocities vs Time&amp;quot; option shows how the internuclear distances are changing in time (i.e. their velocity). An oscillation around zero corresponds to a vibration, while average positive or negative values correspond to two atoms distancing or approach each other respectively.&lt;br /&gt;
&lt;br /&gt;
* Next, select “Energy vs Time” in the same menu.  It will show an oscillatory behaviour rising in energy until the transition state is reached. The potential energy then falls as the trajectory moves into the product / exit channel. The energy is continually switching from potential energy to kinetic energy during the trajectory. Total energy should be conserved, so if you see a decay in the total energy try using a smaller time step. At the turning point of a trajectory, one is at the maxima of the oscillations. At the bottom of the trough of the oscillations the potential energy is low and the molecule is moving faster so the energy has gone into kinetic energy. In this case the kinetic energy reaches its &#039;&#039;minimum&#039;&#039; value at the transition state.&lt;br /&gt;
&lt;br /&gt;
* Finally the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t),  can be displayed using “Momenta vs Time”. This result is not so easy to interpret because the momenta correspond to bond stretching displacements &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; &#039;&#039;&#039;and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; &#039;&#039;&#039;, not the momenta of the atoms themselves.&lt;br /&gt;
&lt;br /&gt;
[[File:Y2C8.png|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Thus &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; is the momentum in the coordinate &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;. Notice that the momentum in the atom 2 results from both momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;.   Thus if we want to collide atom 3 with 1-2 (by giving some &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) in such a way that the diatom 1-2 does not vibrate, we must give some momentum in &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; as well. Following the momentum distribution approaching transition state region and then distancing from it, provides some insight on the distribution of the kinetic energy on the different motions of the system, as we now discuss.&lt;br /&gt;
&lt;br /&gt;
Initially &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(0)=0 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(0)=-2.7.  At the beginning of the trajectory &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) decreases in absolute value and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) takes on an oscillatory behaviour. &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) oscillates because the initial momentum in &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; also forces &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; to change as shown by the picture above. After the transition state at t=0.38, &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) rises rapidly and remains constant (corresponding to translation) as &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; becomes large as H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; leaves.  In contrast &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; &#039;&#039;&#039;initially corresponds to translation. After the transition state &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; oscillates (corresponding to vibration).           &lt;br /&gt;
&lt;br /&gt;
=== Dynamics from the transition state region ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div id=&amp;quot;saddle&amp;quot;&amp;gt;&lt;br /&gt;
[[File:Y2C9.png|thumb|700px|none|Gradients at the transition state, as well as in the reactants and product regions.]]&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;&#039;transition state&#039;&#039;&#039; is defined as the &#039;&#039;maximum&#039;&#039; on the &#039;&#039;&#039;minimum energy path&#039;&#039;&#039; linking reactants and the products. This point on the potential energy surface has the special property that ∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 (the gradient of the potential is zero), and the energy goes down most steeply along the minimum energy path linking reactants and products. Consequently, if one starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever.  However, if one changes the geometry by a small amount in the direction of the products it will roll towards the products (and similarly for the reactants).  One way of locating the transition state is to start trajectories near the transition state and see whether they &amp;quot;roll&amp;quot; towards the reactants or products.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|blue|On a potential energy surface diagram, how is the transition state mathematically defined?&lt;br /&gt;
How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?}}&lt;br /&gt;
&lt;br /&gt;
==== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: locating the transition state ====&lt;br /&gt;
Since the H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;.  If we start a trajectory [[#saddle|on the ridge]] &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; &#039;&#039;&#039;there is no gradient in the direction at right angles to the ridge, thus the trajectory will oscillate on the ridge and never fall off. This fact can be used to locate the TS geometry.&lt;br /&gt;
&lt;br /&gt;
* Locate the transition state of the reactions by testing different initial conditions with &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;  = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;, and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.0.&lt;br /&gt;
&lt;br /&gt;
If you select “Animation” mode, you should see that the system undergoes a periodic symmetric vibration.&lt;br /&gt;
&lt;br /&gt;
[[File:Y2C10.png|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|blue|Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.}}&lt;br /&gt;
&lt;br /&gt;
==== Calculating the reaction path ====&lt;br /&gt;
The &#039;&#039;reaction path&#039;&#039; (minimum energy path or &#039;&#039;mep&#039;&#039;) is a very special trajectory that corresponds to infinitely slow motion (i.e. the momenta/velocities are always reset to zero in each time step). Once the transition state has been located, one may run the very special “trajectory” that corresponds to the &#039;&#039;mep&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
* Set the initial conditions such that the system is slightly displaced from the transition state and zero initial momenta (i.e. the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;+0.01,  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039; and the momenta &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0), then change the calculation type from dynamics to MEP (you may need to increase the number and/or size of steps to obtain a complete mep).&lt;br /&gt;
&lt;br /&gt;
You will see that the trajectory simply follows the valley floor to H&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Trajectories from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+δ, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
While the &#039;&#039;mep&#039;&#039; is useful to characterise a given chemical reaction, it does not provide a realistic account of the motion of the atoms during the reaction. Atoms have mass and in the gas phase (as we are studying here) their motion will be inertial.&lt;br /&gt;
&lt;br /&gt;
* Repeat the calculation with the same initial conditions used to calculate the reaction path, but change the calculation type back to Dynamics.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|blue|Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.}}&lt;br /&gt;
&lt;br /&gt;
Look at the “Internuclear Distances vs Time” and “Momenta vs Time”. What would change if we used the initial conditions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039; and  &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = &#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;+0.01 instead?&lt;br /&gt;
&lt;br /&gt;
Take note of the final values of the positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) and  &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039;(t) for your trajectory for large enough t.&lt;br /&gt;
&lt;br /&gt;
* &amp;lt;div id=&amp;quot;invert momenta&amp;quot;&amp;gt;Setup a calculation where the initial positions correspond to the final positions of the trajectory you calculated above, the same final momenta values but with their signs reversed.&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
What do you observe?&lt;br /&gt;
&lt;br /&gt;
=== Reactive and unreactive trajectories ===&lt;br /&gt;
Is there a general way to determine the conditions for a reactive trajectory that starts in the region of the reactants and passes near the TS region? From the previous calculations we can conclude that trajectories with initial conditions in the range &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74, &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, with -1.5 &amp;lt; &#039;&#039;&#039;p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; &amp;lt; -0.8 and &#039;&#039;&#039;p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = -2.5 are reactive (you can run trajectories yourself to confirm this statement). It would seem fair to assume that all trajectories starting with the same positions but with higher values of momenta (higher kinetic energy) would be reactive, as they have enough kinetic energy to overcome the activation barrier. Let us test this hypothesis.&lt;br /&gt;
&lt;br /&gt;
* For the initial positions &#039;&#039;&#039;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 0.74 and &#039;&#039;&#039;r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039;&#039; = 2.0, run trajectories with the following momenta combination and complete the table.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! 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;
| -1.25 || -2.5  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  || || || ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|blue|Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?}}&lt;br /&gt;
&lt;br /&gt;
The penultimate set of conditions illustrates a case of barrier recrossing. The system crosses the transition state region, you should see the bond in the product actually forms (see “Animation”) but then the system reverts back to the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:Y2C11.png|thumb|600px|none|Trajectory that re-crosses the TS region]]&lt;br /&gt;
&lt;br /&gt;
{{fontcolor|blue|State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?}}&lt;br /&gt;
&lt;br /&gt;
== EXERCISE 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
Select the F - H - H potential surface by changing the atom types in the GUI.&lt;br /&gt;
&lt;br /&gt;
===PES inspection===&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|blue|By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?}}&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|blue|Locate the approximate position of the transition state.}}&lt;br /&gt;
&lt;br /&gt;
Because the activation energy for one of the reactions is so small, it is not easy to locate the transition state immediately. Use the Hammond postulate to guide your search.&lt;br /&gt;
&lt;br /&gt;
{{fontcolor1|blue|Report the activation energy for both reactions.}}&lt;br /&gt;
&lt;br /&gt;
You will be able to report a reasonable estimate by performing a mep (with a sufficient number of steps) from a structure neighbouring the transition state, and choosing to plot the appropriate quantity as a function of &amp;quot;time&amp;quot;.&lt;br /&gt;
&lt;br /&gt;
=== Reaction dynamics ===&lt;br /&gt;
* Identify a set of initial conditions that results in a reactive trajectory for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, and look at the “Animation” and “Momenta vs Time”. {{fontcolor1|blue|In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.}}&lt;br /&gt;
&lt;br /&gt;
* Setup a calculation starting on the side of the reactants of F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, at the bottom of the well r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74, with a momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.5, and explore several values of p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; in the range -3 to 3 (explore values also close to these limits). What do you observe? Note that we are putting a significant amount of energy (much more than the activation energy) into the system on the H - H vibration.&lt;br /&gt;
&lt;br /&gt;
* For the same initial position, increase slightly the momentum p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.8, and considerably reduce the overall energy of the system by reducing the momentum p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.1. What do you observe now?&lt;br /&gt;
&lt;br /&gt;
Let us now focus on the reverse reaction, H + HF.&lt;br /&gt;
&lt;br /&gt;
* Setup initial conditions starting at the bottom of the entry channel, with very low vibrational motion on on the H - F bond, and an arbitrarily high value of p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; above the activation energy (an H atom colliding with a high kinetic energy).&lt;br /&gt;
&lt;br /&gt;
* Try to obtain a reactive trajectory by decreasing the momentum of the incoming H atom and increasing the energy of the H - F vibration. (It may be difficult to find the initial conditions that generate a reactive trajectory for this reaction. Using the [[#invert momenta|inversion of momentum procedure]] for a trajectory starting on the transition state can be useful in this case. Working on the Skew Plot framework could also be helpful.)&lt;br /&gt;
&lt;br /&gt;
The cases studied are an illustration of Polanyi&#039;s empirical rules. {{fontcolor|blue|Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.}}&lt;br /&gt;
&lt;br /&gt;
== Background reading ==&lt;br /&gt;
&amp;lt;div id=&amp;quot;bibliography&amp;quot;&amp;gt;&lt;br /&gt;
Note that it is possible to start this exercise and run some trajectories very easily but reference to literature will be needed to understand the concepts introduced.&lt;br /&gt;
&lt;br /&gt;
===Kinetics/reaction dynamics references===&lt;br /&gt;
A good reference about transition state theory is chapter 10 of J. I. Steinfeld, J. S. Francisco, W. L. Hase [https://imp-primo.hosted.exlibrisgroup.com/primo-explore/fulldisplay?docid=44IMP_ALMA_DS2140126070001591&amp;amp;vid=ICL_VU1 Chemical Kinetic and Dynamics] Prentice-Hall.&lt;br /&gt;
* Chapter 10: Statistical Approach to Reaction Dynamics: Transition State Theory&lt;br /&gt;
** 10.1 - Motion on potential energy surfaces&lt;br /&gt;
** 10.2 - Basic postulates and standard derivation of Transition State Theory&lt;br /&gt;
** 10.3 - Dynamical derivation of Transition State Theory&lt;br /&gt;
** 10.9 - Critique of Transition State Theory&lt;br /&gt;
Also interesting are sections:&lt;br /&gt;
* 9.4 - Some general principles concerning energy disposition in chemical reactions (A discussion of Polanyi&#039;s rules)&lt;br /&gt;
* 8.3.1 - Classical trajectory calculations (A somewhat high level discussion of dynamics and skewed coordinates)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
A somewhat simplified approach can be found in M. J. Pilling, P. W. Seakins [https://imp-primo.hosted.exlibrisgroup.com/primo-explore/fulldisplay?docid=44IMP_ALMA_DS2142087200001591&amp;amp;vid=ICL_VU1 Reaction Kinetics], 2nd edition, OUP, 1995, in particular section:&lt;br /&gt;
* 3.4 - Transition State Theory&lt;br /&gt;
* 4.4 - Reaction dynamics and potential energy surfaces (with a discussion of skewed coordinates)&lt;br /&gt;
* 4.5 - Potential energy surfaces&lt;br /&gt;
* 4.6 - Calculation of kinetic properties from potential energy surfaces&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
A good high level reference for this experiment is D. M. Hirst [https://library-search.imperial.ac.uk/primo-explore/fulldisplay?docid=44IMP_ALMA_DS2146161660001591&amp;amp;vid=ICL_VU1 Potential Energy Surfaces: Molecular Structure and Reaction Dynamics] Taylor and Francis, 1985, in particular section:&lt;br /&gt;
* 6.3 - The relationship between reaction dynamics and potential surface (includes some discussion of Polanyi&#039;s rules and skewed coordinates)&lt;br /&gt;
Also interesting might be:&lt;br /&gt;
* 3.1 - Potential hypersurfaces for triatomic molecules&lt;br /&gt;
* 3.2 - Correlation diagrams&lt;br /&gt;
* 5.4.1 - The London-Eyring-Polanyi-Sato function (a description of the potential energy function we are using)&lt;br /&gt;
* 6.2 -Classical trajectory calculations&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
A very succinct reference, if you like that style, is G. D. Billing, K. V. Mikkelsen [https://imp-primo.hosted.exlibrisgroup.com/primo-explore/fulldisplay?docid=44IMP_ALMA_DS2138844830001591 Introduction to molecular dynamics and chemical kinetics] Willey, 1996.&lt;br /&gt;
* 2 - Interaction potential&lt;br /&gt;
* 3 - Relative motion&lt;br /&gt;
* 5 - Partition functions&lt;br /&gt;
* 6 - Transition State Theory&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For an accessible comment on the derivation of Transition State Theory (or Activated Complex Theory) rate constant expressions see [http://dx.doi.org/10.1021/ed051p709 B. H. Mahan J. Chem. Educ. 51(11):709 (1974)].&lt;br /&gt;
&lt;br /&gt;
===General references===&lt;br /&gt;
Atkins, de Paula, Keeler: [https://library-search.imperial.ac.uk/primo-explore/fulldisplay?docid=44IMP_ALMA_DS5191444090001591&amp;amp;context=L&amp;amp;vid=ICL_VU1&amp;amp;search_scope=LRSCOP_44IMP&amp;amp;isFrbr=true&amp;amp;tab=all&amp;amp;lang=en_US Physical Chemistry], 11&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; Edition.&lt;br /&gt;
* Focus 17: Chemical kinetics&lt;br /&gt;
** Section 17D.2 - The interpretation of Arrhenius parameters&lt;br /&gt;
* Focus 18 Reaction dynamics&lt;br /&gt;
** Section 18A.1 Reactive encounters&lt;br /&gt;
** Section 18C.1 The Eyring Equation (The treatment followed here is not the most relevant for the current experiment and can be confusing. You may want to skip this section and search another reference)&lt;br /&gt;
** Section 18D.2 Reactive collisions&lt;br /&gt;
** Section 18D.3 Potential Energy Surfaces (PESs)&lt;br /&gt;
** Section 18D.4 Some results from experiments and calculations&lt;br /&gt;
&lt;br /&gt;
A good reference is I. N. Levine, [http://imp-primo.hosted.exlibrisgroup.com/ICL_VU1:LRSCOP_44IMP:44IMP_ALMA_DS2145864520001591 Physical Chemistry], McGraw-Hill (section numbers are from the 4th edition).&lt;br /&gt;
* Chapter 23: Theories of reaction rates&lt;br /&gt;
** 23.2: Potential-Energy Surfaces&lt;br /&gt;
** 23.3: Molecular Reaction Dynamics&lt;br /&gt;
** 23.4: Transition State Theory for Ideal-Gas Reactions&lt;br /&gt;
&lt;br /&gt;
If you don&#039;t find the reference above in the library, you can have a look at R. J. Silbey, R. A. Alberty, M. G. Bawendi [http://imp-primo.hosted.exlibrisgroup.com/ICL_VU1:LRSCOP_44IMP:44IMP_ALMA_DS2143891080001591 Physical Chemistry], 4th ed.,  John Wiley &amp;amp; Sons, 2005.&lt;br /&gt;
* Chapter 19: Chemical Dynamics and Photochemistry&lt;br /&gt;
** 19.2: Potential energy surfaces&lt;br /&gt;
** 19.3: Theoretical calculation of a rate constant&lt;br /&gt;
** 19.4: Transition State Theory&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=778741</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=778741"/>
		<updated>2019-05-14T19:05:08Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as the maximum on the minimum energy path. It is defined as the second derivative of the potential energy curve. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=778733</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=778733"/>
		<updated>2019-05-14T19:02:10Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as the maximum on the minimum energy path. It is defined as the second derivative of the potential energy curve. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred. &lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Pp47171.png&amp;diff=778730</id>
		<title>File:Pp47171.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Pp47171.png&amp;diff=778730"/>
		<updated>2019-05-14T19:00:52Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=778728</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=778728"/>
		<updated>2019-05-14T19:00:02Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as the maximum on the minimum energy path. It is defined as the second derivative of the potential energy curve. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-100.619&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton is not transferred. &lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is transferred from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-85.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|no&lt;br /&gt;
|Central proton continuously moves from A to B.&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.2&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-83.579&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|Central proton is initially attached to A, then B to A.&lt;br /&gt;
|&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=778318</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=778318"/>
		<updated>2019-05-14T16:07:28Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as the maximum on the minimum energy path. It is defined as the second derivative of the potential energy curve. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p1&lt;br /&gt;
!p2&lt;br /&gt;
!E(total)&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.25&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-99.119&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|yes&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-1.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.5&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.0&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=778274</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=778274"/>
		<updated>2019-05-14T16:00:52Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as the maximum on the minimum energy path. It is defined as the second derivative of the potential energy curve. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;br /&gt;
&lt;br /&gt;
Comment on how the mep and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
MEP does not consider the momentum that the molecule already has, only the momentum that was defined in the initial conditions in the first step. In the dynamic trajectory, the residual momentum is considered which is why there are vibrations present and the point at which the potential energy is zero occurs at a larger distance.&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=777772</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=777772"/>
		<updated>2019-05-14T15:08:23Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as the maximum on the minimum energy path. It is defined as the second derivative of the potential energy curve. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075 Ǎ&lt;br /&gt;
&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;br /&gt;
&lt;br /&gt;
The Internuclear Distances vs Time plot shows two straight lines corresponding to the bonds A-C and B-C which helped to identify the transition state. There are no fluctuations of the distance with time of the bonds in the transition state because they have no potential energy.&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=777694</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=777694"/>
		<updated>2019-05-14T14:58:24Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
The transition state is mathematically defined as the maximum on the minimum energy path. It is defined as the second derivative of the potential energy curve. &lt;br /&gt;
&lt;br /&gt;
Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&lt;br /&gt;
&lt;br /&gt;
The best transition state position was 0.9075&lt;br /&gt;
[[File:TSpp4717.PNG]]&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:TSpp4717.PNG&amp;diff=777689</id>
		<title>File:TSpp4717.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:TSpp4717.PNG&amp;diff=777689"/>
		<updated>2019-05-14T14:57:49Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=777356</id>
		<title>MRD:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:pp4717&amp;diff=777356"/>
		<updated>2019-05-14T13:28:24Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: Created page with &amp;quot;2nd year computational labs&amp;quot;&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;2nd year computational labs&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776384</id>
		<title>Rep:Mod:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776384"/>
		<updated>2019-05-10T16:13:49Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;b&amp;gt; BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 3-21G&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.46226&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_opt.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000220     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000106     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000940     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000447     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.672478D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.61532&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_631_sum.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000012     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000008     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000061     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.069047D-09&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Low frequencies ---   -0.2263   -0.1037   -0.0054   47.9770   49.0378   49.0383&lt;br /&gt;
 Low frequencies --- 1163.7209 1213.6704 1213.6731&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Vibration&lt;br /&gt;
!Intensity&lt;br /&gt;
!Symmetry&lt;br /&gt;
!IR active&lt;br /&gt;
!Type of vibration&lt;br /&gt;
|-&lt;br /&gt;
|1&lt;br /&gt;
|1164&lt;br /&gt;
|92&lt;br /&gt;
|symmetric&lt;br /&gt;
|yes&lt;br /&gt;
|stretch&lt;br /&gt;
|-&lt;br /&gt;
|2&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|asymmetric&lt;br /&gt;
|yes&lt;br /&gt;
|bend&lt;br /&gt;
|-&lt;br /&gt;
|3&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|asymmetric&lt;br /&gt;
|yes&lt;br /&gt;
|bend&lt;br /&gt;
|-&lt;br /&gt;
|4&lt;br /&gt;
|2580&lt;br /&gt;
|0&lt;br /&gt;
|symmetric&lt;br /&gt;
|no&lt;br /&gt;
|n/a&lt;br /&gt;
|-&lt;br /&gt;
|5&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|symmetric&lt;br /&gt;
|yes&lt;br /&gt;
|bend&lt;br /&gt;
|-&lt;br /&gt;
|6&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|asymmetric&lt;br /&gt;
|yes&lt;br /&gt;
|stretch&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; IR Spectrum &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:IRspec.png|550px]]&lt;br /&gt;
&lt;br /&gt;
There are less than 6 peaks seen in the IR spectrum because 1 peak is not IR active and there are are 2 sets of degenerate frequencies which thus show up as the same peak in the spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MO diagram of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
There are no significant differences in the LCAOs and the computed MOs; this shows the usefulness of the qualititative MO diagram.&lt;br /&gt;
&lt;br /&gt;
[[File:MO.png|600px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_631g.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000060     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000040     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000369     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000162     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.259212D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:amm_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -32.4128  -32.3999  -11.4544   -0.0032    0.0078    0.0521&lt;br /&gt;
 Low frequencies --- 1088.7642 1694.0248 1694.0252&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3bh3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000137     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000038     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001017     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000224     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.131227D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_bh3freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0172   -0.0141   -0.0074  100.7930  100.7958  165.6168&lt;br /&gt;
 Low frequencies ---  421.7202  601.9051  685.5876&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NH3BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Energy Calculation &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55777 a.u&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -26.61532 a.u&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22415 a.u&lt;br /&gt;
&lt;br /&gt;
N-B bond strength = -83.22145 -(-56.55777+ -26.61532) = -0.05106 a.u&lt;br /&gt;
= -134 kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The N-B bond is a dative covalent bond. It is a relatively weak bond compared to the bond strength of C-N which is 305 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NI&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: GEN&lt;br /&gt;
&lt;br /&gt;
[[File:ni3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000114     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000735     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000543     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.081659D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:ni3_pp.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.7242  -12.7182   -6.3942   -0.0039    0.0189    0.0623&lt;br /&gt;
 Low frequencies ---  101.0680  101.0688  147.4487&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NI3 MIXEDPP FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NI3 MIXEDPP FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Optimised N-I bond length: 2.18368&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;b&amp;gt; Ionic Liquids: Designer Solvents &amp;lt;/b&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000132     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000049     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001021     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000301     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.883750D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3 freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0013   -0.0013   -0.0009   32.7135   32.7135   32.7135&lt;br /&gt;
 Low frequencies ---  213.0784  313.6512  313.6512&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NCH34 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NCH34 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3).PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000058     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000016     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000663     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000249     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-5.209118D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt; &lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3) freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---    0.0010    0.0012    0.0015   50.3813   50.3813   50.3813&lt;br /&gt;
 Low frequencies ---  185.7545  210.8019  210.8019&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA PH3NH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA PH3NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NBO Charge distribution: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:N(ch3)4nbo.PNG|700px]]  [[File:P(ch3)4nbo.PNG|700px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The NBO charge analysis of N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; and P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; are differemt because they show a postive charge subsided on the phosphorus atom but a negative charge on the nitrogen atom. &lt;br /&gt;
The magnitude of the charges are also different; the magnitude of charge on the phosphorus atom is 1.667 which is much larger than the magnitude on the nitrogen atom (0.295). This shows that the phosphorus atom is more charged.&lt;br /&gt;
&lt;br /&gt;
The traditional description of the positive charge on the nitrogen centre in the molecule N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is flawed by the NBO analysis. The NBO analysis shows a negative charge on the nitrogen atom and positive charges on the hydrogen atoms. In reality however the charges are not localised; they are distributed around the whole molecule.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MOs from N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:LCAOS.PNG]]&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776375</id>
		<title>Rep:Mod:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776375"/>
		<updated>2019-05-10T16:12:39Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;b&amp;gt; BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 3-21G&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.46226&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_opt.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000220     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000106     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000940     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000447     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.672478D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.61532&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_631_sum.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000012     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000008     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000061     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.069047D-09&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Low frequencies ---   -0.2263   -0.1037   -0.0054   47.9770   49.0378   49.0383&lt;br /&gt;
 Low frequencies --- 1163.7209 1213.6704 1213.6731&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Vibration&lt;br /&gt;
!Intensity&lt;br /&gt;
!Symmetry&lt;br /&gt;
!IR active&lt;br /&gt;
!Type of vibration&lt;br /&gt;
|-&lt;br /&gt;
|1&lt;br /&gt;
|1164&lt;br /&gt;
|92&lt;br /&gt;
|symmetric&lt;br /&gt;
|yes&lt;br /&gt;
|stretch&lt;br /&gt;
|-&lt;br /&gt;
|2&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|asymmetric&lt;br /&gt;
|yes&lt;br /&gt;
|bend&lt;br /&gt;
|-&lt;br /&gt;
|3&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|asymmetric&lt;br /&gt;
|yes&lt;br /&gt;
|bend&lt;br /&gt;
|-&lt;br /&gt;
|4&lt;br /&gt;
|2580&lt;br /&gt;
|0&lt;br /&gt;
|symmetric&lt;br /&gt;
|no&lt;br /&gt;
|n/a&lt;br /&gt;
|-&lt;br /&gt;
|5&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|symmetric&lt;br /&gt;
|yes&lt;br /&gt;
|bend&lt;br /&gt;
|-&lt;br /&gt;
|6&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|asymmetric&lt;br /&gt;
|yes&lt;br /&gt;
|stretch&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; IR Spectrum &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:IRspec.png|550px]]&lt;br /&gt;
&lt;br /&gt;
There are less than 6 peaks seen in the IR spectrum because 1 peak is not IR active and there are are 2 sets of degenerate frequencies which thus show up as the same peak in the spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MO diagram of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
There are no significant differences in the LCAOs and the computed MOs; this shows the usefulness of the qualititative MO diagram.&lt;br /&gt;
&lt;br /&gt;
[[File:MO.png|600px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_631g.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000060     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000040     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000369     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000162     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.259212D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:amm_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -32.4128  -32.3999  -11.4544   -0.0032    0.0078    0.0521&lt;br /&gt;
 Low frequencies --- 1088.7642 1694.0248 1694.0252&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3bh3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000137     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000038     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001017     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000224     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.131227D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_bh3freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0172   -0.0141   -0.0074  100.7930  100.7958  165.6168&lt;br /&gt;
 Low frequencies ---  421.7202  601.9051  685.5876&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NH3BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Energy Calculation &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55777 a.u&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -26.61532 a.u&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22415 a.u&lt;br /&gt;
&lt;br /&gt;
N-B bond strength = -83.22145 -(-56.55777+ -26.61532) = -0.05106 a.u&lt;br /&gt;
= -134 kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The N-B bond is a dative covalent bond. It is a relatively weak bond compared to the bond strength of C-N which is 305 kJ/mol&lt;br /&gt;
&amp;lt;b&amp;gt; NI&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: GEN&lt;br /&gt;
&lt;br /&gt;
[[File:ni3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000114     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000735     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000543     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.081659D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:ni3_pp.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.7242  -12.7182   -6.3942   -0.0039    0.0189    0.0623&lt;br /&gt;
 Low frequencies ---  101.0680  101.0688  147.4487&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NI3 MIXEDPP FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NI3 MIXEDPP FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Optimised N-I bond length: 2.18368&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;b&amp;gt; Ionic Liquids: Designer Solvents &amp;lt;/b&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000132     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000049     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001021     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000301     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.883750D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3 freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0013   -0.0013   -0.0009   32.7135   32.7135   32.7135&lt;br /&gt;
 Low frequencies ---  213.0784  313.6512  313.6512&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NCH34 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NCH34 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3).PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000058     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000016     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000663     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000249     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-5.209118D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt; &lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3) freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---    0.0010    0.0012    0.0015   50.3813   50.3813   50.3813&lt;br /&gt;
 Low frequencies ---  185.7545  210.8019  210.8019&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA PH3NH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA PH3NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NBO Charge distribution: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:N(ch3)4nbo.PNG|700px]]  [[File:P(ch3)4nbo.PNG|700px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The NBO charge analysis of N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; and P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; are differemt because they show a postive charge subsided on the phosphorus atom but a negative charge on the nitrogen atom. &lt;br /&gt;
The magnitude of the charges are also different; the magnitude of charge on the phosphorus atom is 1.667 which is much larger than the magnitude on the nitrogen atom (0.295). This shows that the phosphorus atom is more charged.&lt;br /&gt;
&lt;br /&gt;
The traditional description of the positive charge on the nitrogen centre in the molecule N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is flawed by the NBO analysis. The NBO analysis shows a negative charge on the nitrogen atom and positive charges on the hydrogen atoms. In reality however the charges are not localised; they are distributed around the whole molecule.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MOs from N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:LCAOS.PNG]]&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776307</id>
		<title>Rep:Mod:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776307"/>
		<updated>2019-05-10T16:01:16Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;b&amp;gt; BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 3-21G&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.46226&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_opt.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000220     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000106     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000940     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000447     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.672478D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.61532&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_631_sum.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000012     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000008     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000061     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.069047D-09&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Low frequencies ---   -0.2263   -0.1037   -0.0054   47.9770   49.0378   49.0383&lt;br /&gt;
 Low frequencies --- 1163.7209 1213.6704 1213.6731&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Vibration&lt;br /&gt;
!Intensity&lt;br /&gt;
!Symmetry&lt;br /&gt;
!IR active&lt;br /&gt;
!Type of vibration&lt;br /&gt;
|-&lt;br /&gt;
|1&lt;br /&gt;
|1164&lt;br /&gt;
|92&lt;br /&gt;
|symmetric&lt;br /&gt;
|yes&lt;br /&gt;
|stretch&lt;br /&gt;
|-&lt;br /&gt;
|2&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|asymmetric&lt;br /&gt;
|yes&lt;br /&gt;
|bend&lt;br /&gt;
|-&lt;br /&gt;
|3&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|asymmetric&lt;br /&gt;
|yes&lt;br /&gt;
|bend&lt;br /&gt;
|-&lt;br /&gt;
|4&lt;br /&gt;
|2580&lt;br /&gt;
|0&lt;br /&gt;
|symmetric&lt;br /&gt;
|no&lt;br /&gt;
|n/a&lt;br /&gt;
|-&lt;br /&gt;
|5&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|symmetric&lt;br /&gt;
|yes&lt;br /&gt;
|bend&lt;br /&gt;
|-&lt;br /&gt;
|6&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|asymmetric&lt;br /&gt;
|yes&lt;br /&gt;
|stretch&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; IR Spectrum &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:IRspec.png|550px]]&lt;br /&gt;
&lt;br /&gt;
There are less than 6 peaks seen in the IR spectrum because 1 peak is not IR active and there are are 2 sets of degenerate frequencies which thus show up as the same peak in the spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MO diagram of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
There are no significant differences in the LCAOs and the computed MOs; this shows the usefulness of the qualititative MO diagram.&lt;br /&gt;
&lt;br /&gt;
[[File:MO.png|600px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_631g.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000060     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000040     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000369     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000162     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.259212D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:amm_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -32.4128  -32.3999  -11.4544   -0.0032    0.0078    0.0521&lt;br /&gt;
 Low frequencies --- 1088.7642 1694.0248 1694.0252&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3bh3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000137     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000038     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001017     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000224     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.131227D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_bh3freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0172   -0.0141   -0.0074  100.7930  100.7958  165.6168&lt;br /&gt;
 Low frequencies ---  421.7202  601.9051  685.5876&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NH3BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Energy Calculation &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55777 a.u&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -26.61532 a.u&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22415 a.u&lt;br /&gt;
&lt;br /&gt;
Enthalpy change for the reaction = -83.22145 -(-56.55777+ -26.61532) = -0.05106 a.u&lt;br /&gt;
= -134 kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NI&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: GEN&lt;br /&gt;
&lt;br /&gt;
[[File:ni3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000114     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000735     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000543     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.081659D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:ni3_pp.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.7242  -12.7182   -6.3942   -0.0039    0.0189    0.0623&lt;br /&gt;
 Low frequencies ---  101.0680  101.0688  147.4487&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NI3 MIXEDPP FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NI3 MIXEDPP FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Optimised N-I bond length: 2.18368&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;b&amp;gt; Ionic Liquids: Designer Solvents &amp;lt;/b&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000132     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000049     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001021     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000301     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.883750D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3 freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0013   -0.0013   -0.0009   32.7135   32.7135   32.7135&lt;br /&gt;
 Low frequencies ---  213.0784  313.6512  313.6512&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NCH34 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NCH34 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3).PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000058     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000016     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000663     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000249     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-5.209118D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt; &lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3) freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---    0.0010    0.0012    0.0015   50.3813   50.3813   50.3813&lt;br /&gt;
 Low frequencies ---  185.7545  210.8019  210.8019&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA PH3NH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA PH3NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NBO Charge distribution: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:N(ch3)4nbo.PNG|700px]]  [[File:P(ch3)4nbo.PNG|700px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The NBO charge analysis of N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; and P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; are differemt because they show a postive charge subsided on the phosphorus atom but a negative charge on the nitrogen atom. &lt;br /&gt;
The magnitude of the charges are also different; the magnitude of charge on the phosphorus atom is 1.667 which is much larger than the magnitude on the nitrogen atom (0.295). This shows that the phosphorus atom is more charged.&lt;br /&gt;
&lt;br /&gt;
The traditional description of the positive charge on the nitrogen centre in the molecule N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is flawed by the NBO analysis. The NBO analysis shows a negative charge on the nitrogen atom and positive charges on the hydrogen atoms. In reality however the charges are not localised; they are distributed around the whole molecule.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MOs from N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:LCAOS.PNG]]&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776252</id>
		<title>Rep:Mod:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776252"/>
		<updated>2019-05-10T15:54:29Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;b&amp;gt; BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 3-21G&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.46226&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_opt.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000220     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000106     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000940     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000447     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.672478D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.61532&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_631_sum.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000012     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000008     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000061     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.069047D-09&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Low frequencies ---   -0.2263   -0.1037   -0.0054   47.9770   49.0378   49.0383&lt;br /&gt;
 Low frequencies --- 1163.7209 1213.6704 1213.6731&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Vibration&lt;br /&gt;
!Intensity&lt;br /&gt;
!Symmetry&lt;br /&gt;
!IR active&lt;br /&gt;
!Type of vibration&lt;br /&gt;
|-&lt;br /&gt;
|1&lt;br /&gt;
|1164&lt;br /&gt;
|92&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|2&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|3&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|4&lt;br /&gt;
|2580&lt;br /&gt;
|0&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|5&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|6&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; IR Spectrum &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:IRspec.png|550px]]&lt;br /&gt;
&lt;br /&gt;
There are less than 6 peaks seen in the IR spectrum because 1 peak is not IR active and there are are 2 sets of degenerate frequencies which thus show up as the same peak in the spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MO diagram of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
There are no significant differences in the LCAOs and the computed MOs; this shows the usefulness of the qualititative MO diagram.&lt;br /&gt;
&lt;br /&gt;
[[File:MO.png|600px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_631g.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000060     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000040     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000369     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000162     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.259212D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:amm_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -32.4128  -32.3999  -11.4544   -0.0032    0.0078    0.0521&lt;br /&gt;
 Low frequencies --- 1088.7642 1694.0248 1694.0252&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3bh3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000137     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000038     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001017     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000224     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.131227D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_bh3freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0172   -0.0141   -0.0074  100.7930  100.7958  165.6168&lt;br /&gt;
 Low frequencies ---  421.7202  601.9051  685.5876&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NH3BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Energy Calculation &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55777 a.u&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -26.61532 a.u&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22415 a.u&lt;br /&gt;
&lt;br /&gt;
Enthalpy change for the reaction = -83.22145 -(-56.55777+ -26.61532) = -0.05106 a.u&lt;br /&gt;
= -134 kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NI&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: GEN&lt;br /&gt;
&lt;br /&gt;
[[File:ni3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000114     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000735     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000543     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.081659D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:ni3_pp.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.7242  -12.7182   -6.3942   -0.0039    0.0189    0.0623&lt;br /&gt;
 Low frequencies ---  101.0680  101.0688  147.4487&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NI3 MIXEDPP FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NI3 MIXEDPP FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Optimised N-I bond length: 2.18368&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;b&amp;gt; Ionic Liquids: Designer Solvents &amp;lt;/b&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000132     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000049     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001021     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000301     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.883750D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3 freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0013   -0.0013   -0.0009   32.7135   32.7135   32.7135&lt;br /&gt;
 Low frequencies ---  213.0784  313.6512  313.6512&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NCH34 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NCH34 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3).PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000058     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000016     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000663     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000249     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-5.209118D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt; &lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3) freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---    0.0010    0.0012    0.0015   50.3813   50.3813   50.3813&lt;br /&gt;
 Low frequencies ---  185.7545  210.8019  210.8019&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA PH3NH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA PH3NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NBO Charge distribution: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:N(ch3)4nbo.PNG|700px]]  [[File:P(ch3)4nbo.PNG|700px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The NBO charge analysis of N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; and P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; are differemt because they show a postive charge subsided on the phosphorus atom but a negative charge on the nitrogen atom. &lt;br /&gt;
The magnitude of the charges are also different; the magnitude of charge on the phosphorus atom is 1.667 which is much larger than the magnitude on the nitrogen atom (0.295). This shows that the phosphorus atom is more charged.&lt;br /&gt;
&lt;br /&gt;
The traditional description of the positive charge on the nitrogen centre in the molecule N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is flawed by the NBO analysis. The NBO analysis shows a negative charge on the nitrogen atom and positive charges on the hydrogen atoms. In reality however the charges are not localised; they are distributed around the whole molecule.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MOs from N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:LCAOS.PNG]]&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776237</id>
		<title>Rep:Mod:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776237"/>
		<updated>2019-05-10T15:52:26Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;b&amp;gt; BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 3-21G&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.46226&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_opt.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000220     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000106     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000940     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000447     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.672478D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.61532&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_631_sum.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000012     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000008     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000061     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.069047D-09&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Low frequencies ---   -0.2263   -0.1037   -0.0054   47.9770   49.0378   49.0383&lt;br /&gt;
 Low frequencies --- 1163.7209 1213.6704 1213.6731&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Vibration&lt;br /&gt;
!Intensity&lt;br /&gt;
!Symmetry&lt;br /&gt;
!IR active&lt;br /&gt;
!Type of vibration&lt;br /&gt;
|-&lt;br /&gt;
|1&lt;br /&gt;
|1164&lt;br /&gt;
|92&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|2&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|3&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|4&lt;br /&gt;
|2580&lt;br /&gt;
|0&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|5&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|6&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; IR Spectrum &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:IRspec.png|550px]]&lt;br /&gt;
&lt;br /&gt;
There are less than 6 peaks seen in the IR spectrum because 1 peak is not IR active and there are are 2 sets of degenerate frequencies which thus show up as the same peak in the spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MO diagram of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
There are no significant differences in the LCAOs and the computed MOs; this shows the usefulness of the qualititative MO diagram.&lt;br /&gt;
&lt;br /&gt;
[[File:MO.png|600px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_631g.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000060     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000040     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000369     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000162     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.259212D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:amm_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -32.4128  -32.3999  -11.4544   -0.0032    0.0078    0.0521&lt;br /&gt;
 Low frequencies --- 1088.7642 1694.0248 1694.0252&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3bh3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000137     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000038     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001017     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000224     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.131227D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_bh3freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0172   -0.0141   -0.0074  100.7930  100.7958  165.6168&lt;br /&gt;
 Low frequencies ---  421.7202  601.9051  685.5876&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NH3BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Energy Calculation &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55777 a.u&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -26.61532 a.u&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22415 a.u&lt;br /&gt;
&lt;br /&gt;
Enthalpy change for the reaction = -83.22145 -(-56.55777+ -26.61532) = -0.05106 a.u&lt;br /&gt;
= -134 kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NI&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: GEN&lt;br /&gt;
&lt;br /&gt;
[[File:ni3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000114     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000735     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000543     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.081659D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:ni3_pp.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.7242  -12.7182   -6.3942   -0.0039    0.0189    0.0623&lt;br /&gt;
 Low frequencies ---  101.0680  101.0688  147.4487&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NI3 MIXEDPP FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NI3 MIXEDPP FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Optimised N-I bond length: 2.18368&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;b&amp;gt; Ionic Liquids: Designer Solvents &amp;lt;/b&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000132     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000049     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001021     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000301     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.883750D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3 freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0013   -0.0013   -0.0009   32.7135   32.7135   32.7135&lt;br /&gt;
 Low frequencies ---  213.0784  313.6512  313.6512&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NCH34.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NCH34 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3).PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000058     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000016     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000663     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000249     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-5.209118D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt; &lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3) freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---    0.0010    0.0012    0.0015   50.3813   50.3813   50.3813&lt;br /&gt;
 Low frequencies ---  185.7545  210.8019  210.8019&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA PH3NH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA PH3NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NBO Charge distribution: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:N(ch3)4nbo.PNG|700px]]  [[File:P(ch3)4nbo.PNG|700px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The NBO charge analysis of N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; and P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; are differemt because they show a postive charge subsided on the phosphorus atom but a negative charge on the nitrogen atom. &lt;br /&gt;
The magnitude of the charges are also different; the magnitude of charge on the phosphorus atom is 1.667 which is much larger than the magnitude on the nitrogen atom (0.295). This shows that the phosphorus atom is more charged.&lt;br /&gt;
&lt;br /&gt;
The traditional description of the positive charge on the nitrogen centre in the molecule N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is flawed by the NBO analysis. The NBO analysis shows a negative charge on the nitrogen atom and positive charges on the hydrogen atoms. In reality however the charges are not localised; they are distributed around the whole molecule.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MOs from N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:LCAOS.PNG]]&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776228</id>
		<title>Rep:Mod:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776228"/>
		<updated>2019-05-10T15:51:25Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;b&amp;gt; BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 3-21G&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.46226&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_opt.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000220     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000106     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000940     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000447     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.672478D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.61532&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_631_sum.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000012     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000008     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000061     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.069047D-09&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Low frequencies ---   -0.2263   -0.1037   -0.0054   47.9770   49.0378   49.0383&lt;br /&gt;
 Low frequencies --- 1163.7209 1213.6704 1213.6731&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Vibration&lt;br /&gt;
!Intensity&lt;br /&gt;
!Symmetry&lt;br /&gt;
!IR active&lt;br /&gt;
!Type of vibration&lt;br /&gt;
|-&lt;br /&gt;
|1&lt;br /&gt;
|1164&lt;br /&gt;
|92&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|2&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|3&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|4&lt;br /&gt;
|2580&lt;br /&gt;
|0&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|5&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|6&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; IR Spectrum &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:IRspec.png|550px]]&lt;br /&gt;
&lt;br /&gt;
There are less than 6 peaks seen in the IR spectrum because 1 peak is not IR active and there are are 2 sets of degenerate frequencies which thus show up as the same peak in the spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MO diagram of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
There are no significant differences in the LCAOs and the computed MOs; this shows the usefulness of the qualititative MO diagram.&lt;br /&gt;
&lt;br /&gt;
[[File:MO.png|600px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_631g.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000060     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000040     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000369     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000162     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.259212D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:amm_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -32.4128  -32.3999  -11.4544   -0.0032    0.0078    0.0521&lt;br /&gt;
 Low frequencies --- 1088.7642 1694.0248 1694.0252&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3bh3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000137     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000038     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001017     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000224     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.131227D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_bh3freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0172   -0.0141   -0.0074  100.7930  100.7958  165.6168&lt;br /&gt;
 Low frequencies ---  421.7202  601.9051  685.5876&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NH3BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Energy Calculation &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55777 a.u&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -26.61532 a.u&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22415 a.u&lt;br /&gt;
&lt;br /&gt;
Enthalpy change for the reaction = -83.22145 -(-56.55777+ -26.61532) = -0.05106 a.u&lt;br /&gt;
= -134 kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NI&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: GEN&lt;br /&gt;
&lt;br /&gt;
[[File:ni3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000114     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000735     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000543     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.081659D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:ni3_pp.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.7242  -12.7182   -6.3942   -0.0039    0.0189    0.0623&lt;br /&gt;
 Low frequencies ---  101.0680  101.0688  147.4487&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NI3 MIXEDPP.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NI3 MIXEDPP FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Optimised N-I bond length: 2.18368&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;b&amp;gt; Ionic Liquids: Designer Solvents &amp;lt;/b&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000132     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000049     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001021     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000301     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.883750D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3 freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0013   -0.0013   -0.0009   32.7135   32.7135   32.7135&lt;br /&gt;
 Low frequencies ---  213.0784  313.6512  313.6512&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA NCH34.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NCH34 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3).PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000058     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000016     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000663     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000249     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-5.209118D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt; &lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3) freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---    0.0010    0.0012    0.0015   50.3813   50.3813   50.3813&lt;br /&gt;
 Low frequencies ---  185.7545  210.8019  210.8019&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA PH3NH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA PH3NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NBO Charge distribution: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:N(ch3)4nbo.PNG|700px]]  [[File:P(ch3)4nbo.PNG|700px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The NBO charge analysis of N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; and P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; are differemt because they show a postive charge subsided on the phosphorus atom but a negative charge on the nitrogen atom. &lt;br /&gt;
The magnitude of the charges are also different; the magnitude of charge on the phosphorus atom is 1.667 which is much larger than the magnitude on the nitrogen atom (0.295). This shows that the phosphorus atom is more charged.&lt;br /&gt;
&lt;br /&gt;
The traditional description of the positive charge on the nitrogen centre in the molecule N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is flawed by the NBO analysis. The NBO analysis shows a negative charge on the nitrogen atom and positive charges on the hydrogen atoms. In reality however the charges are not localised; they are distributed around the whole molecule.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MOs from N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:LCAOS.PNG]]&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776212</id>
		<title>Rep:Mod:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776212"/>
		<updated>2019-05-10T15:48:40Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;b&amp;gt; BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 3-21G&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.46226&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_opt.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000220     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000106     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000940     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000447     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.672478D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.61532&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_631_sum.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000012     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000008     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000061     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.069047D-09&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Low frequencies ---   -0.2263   -0.1037   -0.0054   47.9770   49.0378   49.0383&lt;br /&gt;
 Low frequencies --- 1163.7209 1213.6704 1213.6731&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:PRIYA BH3 FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Vibration&lt;br /&gt;
!Intensity&lt;br /&gt;
!Symmetry&lt;br /&gt;
!IR active&lt;br /&gt;
!Type of vibration&lt;br /&gt;
|-&lt;br /&gt;
|1&lt;br /&gt;
|1164&lt;br /&gt;
|92&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|2&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|3&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|4&lt;br /&gt;
|2580&lt;br /&gt;
|0&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|5&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|6&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; IR Spectrum &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:IRspec.png|550px]]&lt;br /&gt;
&lt;br /&gt;
There are less than 6 peaks seen in the IR spectrum because 1 peak is not IR active and there are are 2 sets of degenerate frequencies which thus show up as the same peak in the spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MO diagram of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
There are no significant differences in the LCAOs and the computed MOs; this shows the usefulness of the qualititative MO diagram.&lt;br /&gt;
&lt;br /&gt;
[[File:MO.png|600px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_631g.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000060     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000040     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000369     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000162     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.259212D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:amm_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -32.4128  -32.3999  -11.4544   -0.0032    0.0078    0.0521&lt;br /&gt;
 Low frequencies --- 1088.7642 1694.0248 1694.0252&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3bh3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000137     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000038     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001017     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000224     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.131227D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_bh3freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0172   -0.0141   -0.0074  100.7930  100.7958  165.6168&lt;br /&gt;
 Low frequencies ---  421.7202  601.9051  685.5876&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Energy Calculation &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55777 a.u&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -26.61532 a.u&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22415 a.u&lt;br /&gt;
&lt;br /&gt;
Enthalpy change for the reaction = -83.22145 -(-56.55777+ -26.61532) = -0.05106 a.u&lt;br /&gt;
= -134 kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NI&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: GEN&lt;br /&gt;
&lt;br /&gt;
[[File:ni3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000114     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000735     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000543     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.081659D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:ni3_pp.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.7242  -12.7182   -6.3942   -0.0039    0.0189    0.0623&lt;br /&gt;
 Low frequencies ---  101.0680  101.0688  147.4487&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NI3 MIXEDPP FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Optimised N-I bond length: 2.18368&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;b&amp;gt; Ionic Liquids: Designer Solvents &amp;lt;/b&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000132     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000049     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001021     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000301     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.883750D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3 freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0013   -0.0013   -0.0009   32.7135   32.7135   32.7135&lt;br /&gt;
 Low frequencies ---  213.0784  313.6512  313.6512&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NCH34 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3).PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000058     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000016     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000663     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000249     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-5.209118D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt; &lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3) freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---    0.0010    0.0012    0.0015   50.3813   50.3813   50.3813&lt;br /&gt;
 Low frequencies ---  185.7545  210.8019  210.8019&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA PH3NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NBO Charge distribution: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:N(ch3)4nbo.PNG|700px]]  [[File:P(ch3)4nbo.PNG|700px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The NBO charge analysis of N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; and P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; are differemt because they show a postive charge subsided on the phosphorus atom but a negative charge on the nitrogen atom. &lt;br /&gt;
The magnitude of the charges are also different; the magnitude of charge on the phosphorus atom is 1.667 which is much larger than the magnitude on the nitrogen atom (0.295). This shows that the phosphorus atom is more charged.&lt;br /&gt;
&lt;br /&gt;
The traditional description of the positive charge on the nitrogen centre in the molecule N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is flawed by the NBO analysis. The NBO analysis shows a negative charge on the nitrogen atom and positive charges on the hydrogen atoms. In reality however the charges are not localised; they are distributed around the whole molecule.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MOs from N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:LCAOS.PNG]]&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776156</id>
		<title>Rep:Mod:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776156"/>
		<updated>2019-05-10T15:43:53Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;b&amp;gt; BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 3-21G&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.46226&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_opt.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000220     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000106     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000940     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000447     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.672478D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.61532&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_631_sum.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000012     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000008     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000061     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.069047D-09&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Low frequencies ---   -0.2263   -0.1037   -0.0054   47.9770   49.0378   49.0383&lt;br /&gt;
 Low frequencies --- 1163.7209 1213.6704 1213.6731&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Vibration&lt;br /&gt;
!Intensity&lt;br /&gt;
!Symmetry&lt;br /&gt;
!IR active&lt;br /&gt;
!Type of vibration&lt;br /&gt;
|-&lt;br /&gt;
|1&lt;br /&gt;
|1164&lt;br /&gt;
|92&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|2&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|3&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|4&lt;br /&gt;
|2580&lt;br /&gt;
|0&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|5&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|6&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; IR Spectrum &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:IRspec.png|550px]]&lt;br /&gt;
&lt;br /&gt;
There are less than 6 peaks seen in the IR spectrum because 1 peak is not IR active and there are are 2 sets of degenerate frequencies which thus show up as the same peak in the spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MO diagram of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
There are no significant differences in the LCAOs and the computed MOs; this shows the usefulness of the qualititative MO diagram.&lt;br /&gt;
&lt;br /&gt;
[[File:MO.png|600px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_631g.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000060     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000040     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000369     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000162     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.259212D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:amm_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -32.4128  -32.3999  -11.4544   -0.0032    0.0078    0.0521&lt;br /&gt;
 Low frequencies --- 1088.7642 1694.0248 1694.0252&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3bh3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000137     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000038     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001017     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000224     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.131227D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_bh3freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0172   -0.0141   -0.0074  100.7930  100.7958  165.6168&lt;br /&gt;
 Low frequencies ---  421.7202  601.9051  685.5876&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Energy Calculation &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55777 a.u&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -26.61532 a.u&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22415 a.u&lt;br /&gt;
&lt;br /&gt;
Enthalpy change for the reaction = -83.22145 -(-56.55777+ -26.61532) = -0.05106 a.u&lt;br /&gt;
= -134 kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NI&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: GEN&lt;br /&gt;
&lt;br /&gt;
[[File:ni3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000114     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000735     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000543     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.081659D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:ni3_pp.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.7242  -12.7182   -6.3942   -0.0039    0.0189    0.0623&lt;br /&gt;
 Low frequencies ---  101.0680  101.0688  147.4487&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NI3 MIXEDPP FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Optimised N-I bond length: 2.18368&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;b&amp;gt; Ionic Liquids: Designer Solvents &amp;lt;/b&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000132     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000049     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001021     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000301     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.883750D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3 freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0013   -0.0013   -0.0009   32.7135   32.7135   32.7135&lt;br /&gt;
 Low frequencies ---  213.0784  313.6512  313.6512&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NCH34 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3).PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000058     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000016     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000663     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000249     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-5.209118D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt; &lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3) freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---    0.0010    0.0012    0.0015   50.3813   50.3813   50.3813&lt;br /&gt;
 Low frequencies ---  185.7545  210.8019  210.8019&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA PH3NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NBO Charge distribution: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:N(ch3)4nbo.PNG|700px]]  [[File:P(ch3)4nbo.PNG|700px]]&lt;br /&gt;
&lt;br /&gt;
The NBO charge analysis of N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; and P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; are differemt because they show a postive charge subsided on the phosphorus atom but a negative charge on the nitrogen atom. &lt;br /&gt;
The magnitude of the charges are also different; the magnitude of charge on the phosphorus atom is 1.667 which is much larger than the magnitude on the nitrogen atom (0.295). This shows that the phosphorus atom is more charged.&lt;br /&gt;
&lt;br /&gt;
The traditional description of the positive charge on the nitrogen centre in the molecule N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is flawed by the NBO analysis. The NBO analysis shows a negative charge on the nitrogen atom and positive charges on the hydrogen atoms. In reality however the charges are not localised; they are distributed around the whole molecule.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:LCAOS.PNG]]&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776134</id>
		<title>Rep:Mod:pp4717</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:pp4717&amp;diff=776134"/>
		<updated>2019-05-10T15:40:37Z</updated>

		<summary type="html">&lt;p&gt;Pp4717: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;lt;b&amp;gt; BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 3-21G&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.46226&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_opt.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000220     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000106     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000940     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000447     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.672478D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
Final energy in atomic units (a.u): -26.61532&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_631_sum.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000012     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000008     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000061     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.069047D-09&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:bh3_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Low frequencies ---   -0.2263   -0.1037   -0.0054   47.9770   49.0378   49.0383&lt;br /&gt;
 Low frequencies --- 1163.7209 1213.6704 1213.6731&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Vibration&lt;br /&gt;
!Intensity&lt;br /&gt;
!Symmetry&lt;br /&gt;
!IR active&lt;br /&gt;
!Type of vibration&lt;br /&gt;
|-&lt;br /&gt;
|1&lt;br /&gt;
|1164&lt;br /&gt;
|92&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|2&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|3&lt;br /&gt;
|1214&lt;br /&gt;
|14&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|4&lt;br /&gt;
|2580&lt;br /&gt;
|0&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|5&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|6&lt;br /&gt;
|2713&lt;br /&gt;
|126&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; IR Spectrum &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:IRspec.png|550px]]&lt;br /&gt;
&lt;br /&gt;
There are less than 6 peaks seen in the IR spectrum because 1 peak is not IR active and there are are 2 sets of degenerate frequencies which thus show up as the same peak in the spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; MO diagram of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
There are no significant differences in the LCAOs and the computed MOs; this shows the usefulness of the qualititative MO diagram.&lt;br /&gt;
&lt;br /&gt;
[[File:MO.png|600px]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_631g.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000060     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000040     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000369     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000162     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.259212D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:amm_freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -32.4128  -32.3999  -11.4544   -0.0032    0.0078    0.0521&lt;br /&gt;
 Low frequencies --- 1088.7642 1694.0248 1694.0252&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31G (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:nh3bh3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000137     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000038     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001017     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000224     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.131227D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:nh3_bh3freq.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0172   -0.0141   -0.0074  100.7930  100.7958  165.6168&lt;br /&gt;
 Low frequencies ---  421.7202  601.9051  685.5876&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NH3BH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Energy Calculation &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55777 a.u&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -26.61532 a.u&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22415 a.u&lt;br /&gt;
&lt;br /&gt;
Enthalpy change for the reaction = -83.22145 -(-56.55777+ -26.61532) = -0.05106 a.u&lt;br /&gt;
= -134 kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NI&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: GEN&lt;br /&gt;
&lt;br /&gt;
[[File:ni3.png|260px]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000114     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000735     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000543     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.081659D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:ni3_pp.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.7242  -12.7182   -6.3942   -0.0039    0.0189    0.0623&lt;br /&gt;
 Low frequencies ---  101.0680  101.0688  147.4487&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NI3 MIXEDPP FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Optimised N-I bond length: 2.18368&lt;br /&gt;
&lt;br /&gt;
=== &amp;lt;b&amp;gt; Ionic Liquids: Designer Solvents &amp;lt;/b&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000132     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000049     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001021     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000301     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.883750D-07&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Nch3 freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0013   -0.0013   -0.0009   32.7135   32.7135   32.7135&lt;br /&gt;
 Low frequencies ---  213.0784  313.6512  313.6512&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA NCH34 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; optimisation: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis set: 6-31 (d,p)&lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3).PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000058     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000016     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000663     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000249     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-5.209118D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Frequency analysis: &amp;lt;/b&amp;gt; &lt;br /&gt;
&lt;br /&gt;
[[File:P(ch3) freq.PNG]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---    0.0010    0.0012    0.0015   50.3813   50.3813   50.3813&lt;br /&gt;
 Low frequencies ---  185.7545  210.8019  210.8019&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;PRIYA PH3NH3 FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; NBO Charge distribution: &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:N(ch3)4nbo.PNG|700px]]  [[File:P(ch3)4nbo.PNG|700px]]&lt;br /&gt;
&lt;br /&gt;
The NBO charge analysis of N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; and P(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; are differemt because they show a postive charge subsided on the phosphorus atom but a negative charge on the nitrogen atom. &lt;br /&gt;
&lt;br /&gt;
The traditional description of the positive charge on the nitrogen centre in the molecule N(CH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is flawed by the NBO analysis. The NBO analysis shows a negative charge on the nitrogen atom and positive charges on the hydrogen atoms. In reality however the charges are not localised; they are distributed around the whole molecule.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:LCAOS.PNG]]&lt;/div&gt;</summary>
		<author><name>Pp4717</name></author>
	</entry>
</feed>