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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722811</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722811"/>
		<updated>2018-05-18T14:35:34Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Polanyi&amp;#039;s rules */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.81 Å and BC was 0.75 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
When a transition state is seen, it can mimic the products or reactants; these rules follow the effects of vibrational, and translational, vibrations have on this. &amp;lt;ref name=&amp;quot;[2]&amp;quot; /&amp;gt; It is seen that high vibrational energy leads to an late Ts, with the early Ts being highly disfavoured. Exothermic reactions are late transition states, therefore has products with increased amount of vibrational energy, and lower translational as energy must be conserved. &amp;lt;ref name=&amp;quot;[3]&amp;quot; /&amp;gt; For an endothermic reaction, this is simply reversed. &lt;br /&gt;
&lt;br /&gt;
A set up of AB=1.8 and BC=0.78 were used to see the rules for our exothermic reaction. The momenta were set to -0.55 and 0.15 respectively, followed by a run of the inverse of this. Run 1 showed product being formed, however run 2 showed no product being formed, mainly due to it&#039;s initial momentum being in the wrong direction. This being the exothermic part of the reversible reaction, it has a late transition state, therefore the vibrational energy is seen to show the best efficacy towards driving the reaction on.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Prules run1.PNG | thumb | left | 300px | Run 1]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Prules run2.PNG | thumb | centre | 300px | Run 2]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[2]&amp;quot;&amp;gt;Evans, M. G.; Polanyi, M., J. Chem. Soc., Faraday Trans., 1936, 32, 1340.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[3]&amp;quot;&amp;gt;Z. Zhang et al, J.Phys. Chem. Lett., 2012, &amp;quot;Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction&amp;quot;, Vol. 3 (23) p.3416–3419.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722806</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722806"/>
		<updated>2018-05-18T14:35:05Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Polanyi&amp;#039;s rules */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.81 Å and BC was 0.75 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
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&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
When a transition state is seen, it can mimic the products or reactants; these rules follow the effects of vibrational, and translational, vibrations have on this. &amp;lt;ref name=&amp;quot;[2]&amp;quot; /&amp;gt; It is seen that high vibrational energy leads to an late Ts, with the early Ts being highly disfavoured. Exothermic reactions are late transition states, therefore has products with increased amount of vibrational energy, and lower translational as energy must be conserved. &amp;lt;ref name=&amp;quot;[3]&amp;quot; /&amp;gt; For an endothermic reaction, this is simply reversed. &lt;br /&gt;
&lt;br /&gt;
A set up of AB=1.8 and BC=0.78 were used to see the rules for our exothermic reaction. The momenta were set to -0.55 and 0.15 respectively, followed by a run of the inverse of this. Run 1 showed product being formed, however run 2 showed no product being formed, mainly due to it&#039;s initial momentum being in the wrong direction. This being the exothermic part of the reversible reaction, it has a late transition state, therefore the vibrational energy is seen to show the best efficacy towards driving the reaction on.&lt;br /&gt;
&lt;br /&gt;
[File:HJW116 Prules run1.PNG | thumb | left | 300px | Run 1]]&lt;br /&gt;
&lt;br /&gt;
[File:HJW116 Prules run2.PNG | thumb | centre | 300px | Run 2]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[2]&amp;quot;&amp;gt;Evans, M. G.; Polanyi, M., J. Chem. Soc., Faraday Trans., 1936, 32, 1340.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[3]&amp;quot;&amp;gt;Z. Zhang et al, J.Phys. Chem. Lett., 2012, &amp;quot;Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction&amp;quot;, Vol. 3 (23) p.3416–3419.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:HJW116_Prules_run2.PNG&amp;diff=722734</id>
		<title>File:HJW116 Prules run2.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:HJW116_Prules_run2.PNG&amp;diff=722734"/>
		<updated>2018-05-18T14:26:46Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:HJW116_Prules_run1.PNG&amp;diff=722727</id>
		<title>File:HJW116 Prules run1.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:HJW116_Prules_run1.PNG&amp;diff=722727"/>
		<updated>2018-05-18T14:26:00Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722633</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722633"/>
		<updated>2018-05-18T14:18:30Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.81 Å and BC was 0.75 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
When a transition state is seen, it can mimic the products or reactants; these rules follow the effects of vibrational, and translational, vibrations have on this. &amp;lt;ref name=&amp;quot;[2]&amp;quot; /&amp;gt; It is seen that high vibrational energy leads to an late Ts, with the early Ts being highly disfavoured. Exothermic reactions are late transition states, therefore has products with increased amount of vibrational energy, and lower translational as energy must be conserved. &amp;lt;ref name=&amp;quot;[3]&amp;quot; /&amp;gt; For an endothermic reaction, this is simply reversed. &lt;br /&gt;
&lt;br /&gt;
From this it can be said that translational energy in the reactants affects the efficiency of reactions with an early transition state and that vibrational energy in the reactants affects the efficiency of reactions with a late transition state. [1] This supports Polanyi&#039;s Empirical Rules which states that vibrational energy is more efficient at driving a reaction with a late transition state than translational energy. [2]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[2]&amp;quot;&amp;gt;Evans, M. G.; Polanyi, M., J. Chem. Soc., Faraday Trans., 1936, 32, 1340.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[3]&amp;quot;&amp;gt;Z. Zhang et al, J.Phys. Chem. Lett., 2012, &amp;quot;Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction&amp;quot;, Vol. 3 (23) p.3416–3419.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722614</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722614"/>
		<updated>2018-05-18T14:16:52Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.81 Å and BC was 0.75 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
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&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
When a transition state is seen, it can mimic the products or reactants; these rules follow the effects of vibrational, and translational, vibrations have on this. &amp;lt;ref name=&amp;quot;[2]&amp;quot; /&amp;gt; It is seen that high vibrational energy leads to an late Ts, with the early Ts being highly disfavoured. Exothermic reactions are late transition states, therefore has products with increased amount of vibrational energy, and lower translational as energy must be conserved. &amp;lt;ref name=&amp;quot;[3]&amp;quot; /&amp;gt; For an endothermic reaction, this is simply reversed. &lt;br /&gt;
&lt;br /&gt;
From this it can be said that translational energy in the reactants affects the efficiency of reactions with an early transition state and that vibrational energy in the reactants affects the efficiency of reactions with a late transition state. [1] This supports Polanyi&#039;s Empirical Rules which states that vibrational energy is more efficient at driving a reaction with a late transition state than translational energy. [2]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[2]&amp;quot;&amp;gt;Evans, M. G.; Polanyi, M., J. Chem. Soc., Faraday Trans., 1936, 32, 1340.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[3]&amp;quot;&amp;gt;Z. Zhang et al, J.Phys. Chem. Lett., 2012, &amp;quot;Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction&amp;quot;, Vol. 3 (23) p.3416–3419.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722607</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722607"/>
		<updated>2018-05-18T14:16:27Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Polanyi&amp;#039;s rules */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.81 Å and BC was 0.75 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
When a transition state is seen, it can mimic the products or reactants; these rules follow the effects of vibrational, and translational, vibrations have on this. &amp;lt;ref name=&amp;quot;[2]&amp;quot; /&amp;gt; It is seen that high vibrational energy leads to an late Ts, with the early Ts being highly disfavoured. Exothermic reactions are late transition states, therefore has products with increased amount of vibrational energy, and lower translational as energy must be conserved. &amp;lt;ref name=&amp;quot;[3]&amp;quot; /&amp;gt; For an endothermic reaction, this is simply reversed. &lt;br /&gt;
&lt;br /&gt;
From this it can be said that translational energy in the reactants affects the efficiency of reactions with an early transition state and that vibrational energy in the reactants affects the efficiency of reactions with a late transition state. [1] This supports Polanyi&#039;s Empirical Rules which states that vibrational energy is more efficient at driving a reaction with a late transition state than translational energy. [2]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[3]&amp;quot;&amp;gt;Evans, M. G.; Polanyi, M., J. Chem. Soc., Faraday Trans., 1936, 32, 1340.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[3]&amp;quot;&amp;gt;Z. Zhang et al, J.Phys. Chem. Lett., 2012, &amp;quot;Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction&amp;quot;, Vol. 3 (23) p.3416–3419.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722601</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722601"/>
		<updated>2018-05-18T14:15:48Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.81 Å and BC was 0.75 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
When a transition state is seen, it can mimic the products or reactants; these rules follow the effects of vibrational, and translational, vibrations have on this. &amp;lt;ref name=&amp;quot;[2]&amp;quot;/&amp;gt; It is seen that high vibrational energy leads to an late Ts, with the early Ts being highly disfavoured. Exothermic reactions are late transition states, therefore has products with increased amount of vibrational energy, and lower translational as energy must be conserved. &amp;lt;ref name=&amp;quot;[3]&amp;quot; /&amp;gt; For an endothermic reaction, this is simply reversed. &lt;br /&gt;
&lt;br /&gt;
From this it can be said that translational energy in the reactants affects the efficiency of reactions with an early transition state and that vibrational energy in the reactants affects the efficiency of reactions with a late transition state. [1] This supports Polanyi&#039;s Empirical Rules which states that vibrational energy is more efficient at driving a reaction with a late transition state than translational energy. [2]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[3]&amp;quot;&amp;gt;Evans, M. G.; Polanyi, M., J. Chem. Soc., Faraday Trans., 1936, 32, 1340.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[3]&amp;quot;&amp;gt;Z. Zhang et al, J.Phys. Chem. Lett., 2012, &amp;quot;Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction&amp;quot;, Vol. 3 (23) p.3416–3419.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722599</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722599"/>
		<updated>2018-05-18T14:15:25Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.81 Å and BC was 0.75 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
When a transition state is seen, it can mimic the products or reactants; these rules follow the effects of vibrational, and translational, vibrations have on this. &amp;lt;ref name=&amp;quot;[2]&amp;quot;/&amp;gt; It is seen that high vibrational energy leads to an late Ts, with the early Ts being highly disfavoured. Exothermic reactions are late transition states, therefore has products with increased amount of vibrational energy, and lower translational as energy must be conserved. &amp;lt;ref name=&amp;quot;[3]&amp;quot; /&amp;gt; For an endothermic reaction, this is simply reversed. &lt;br /&gt;
&lt;br /&gt;
From this it can be said that translational energy in the reactants affects the efficiency of reactions with an early transition state and that vibrational energy in the reactants affects the efficiency of reactions with a late transition state. [1] This supports Polanyi&#039;s Empirical Rules which states that vibrational energy is more efficient at driving a reaction with a late transition state than translational energy. [2]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[3]&amp;quot;&amp;gt;Evans, M. G.; Polanyi, M., J. Chem. Soc., Faraday Trans., 1936, 32, 1340&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[3]&amp;quot;&amp;gt;Z. Zhang et al, J.Phys. Chem. Lett., 2012, &amp;quot;Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction&amp;quot;, Vol. 3 (23) p.3416–3419&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722593</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722593"/>
		<updated>2018-05-18T14:14:50Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Polanyi&amp;#039;s rules */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.81 Å and BC was 0.75 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
When a transition state is seen, it can mimic the products or reactants; these rules follow the effects of vibrational, and translational, vibrations have on this. &amp;lt;ref name=&amp;quot;[2]&amp;quot;/&amp;gt; It is seen that high vibrational energy leads to an late Ts, with the early Ts being highly disfavoured. Exothermic reactions are late transition states, therefore has products with increased amount of vibrational energy, and lower translational as energy must be conserved. &amp;lt;ref name=&amp;quot;[3]&amp;quot; /&amp;gt; For an endothermic reaction, this is simply reversed. &lt;br /&gt;
&lt;br /&gt;
From this it can be said that translational energy in the reactants affects the efficiency of reactions with an early transition state and that vibrational energy in the reactants affects the efficiency of reactions with a late transition state. [1] This supports Polanyi&#039;s Empirical Rules which states that vibrational energy is more efficient at driving a reaction with a late transition state than translational energy. [2]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[2]&amp;quot;&amp;gt;Z. Zhang et al, J.Phys. Chem. Lett., 2012, &amp;quot;Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction&amp;quot;, Vol. 3 (23) p.3416–3419.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722501</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722501"/>
		<updated>2018-05-18T14:07:29Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.81 Å and BC was 0.75 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
When a transition state is seen, it can mimic the products or reactants; these rules follow the effects of vibrational, and translational, vibrations have on this. It is seen that high vibrational energy leads to an late Ts, with the early Ts being highly disfavoured. Exothermic reactions are late transition states, therefore has products with increased amount of vibrational energy, and lower translational as energy must be conserved. For an endothermic reaction, this is simply reversed. &lt;br /&gt;
&lt;br /&gt;
From this it can be said that translational energy in the reactants affects the efficiency of reactions with an early transition state and that vibrational energy in the reactants affects the efficiency of reactions with a late transition state. [1] This supports Polanyi&#039;s Empirical Rules which states that vibrational energy is more efficient at driving a reaction with a late transition state than translational energy. [2]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[2]&amp;quot;&amp;gt;Z. Zhang et al, J.Phys. Chem. Lett., 2012, &amp;quot;Theoretical Study of the Validity of the Polanyi Rules for the Late-Barrier Cl + CHD3 Reaction&amp;quot;, Vol. 3 (23) p.3416–3419.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722495</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=722495"/>
		<updated>2018-05-18T14:06:57Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Polanyi&amp;#039;s rules */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.81 Å and BC was 0.75 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
When a transition state is seen, it can mimic the products or reactants; these rules follow the effects of vibrational, and translational, vibrations have on this. It is seen that high vibrational energy leads to an late Ts, with the early Ts being highly disfavoured. Exothermic reactions are late transition states, therefore has products with increased amount of vibrational energy, and lower translational as energy must be conserved. For an endothermic reaction, this is simply reversed. &lt;br /&gt;
&lt;br /&gt;
From this it can be said that translational energy in the reactants affects the efficiency of reactions with an early transition state and that vibrational energy in the reactants affects the efficiency of reactions with a late transition state. [1] This supports Polanyi&#039;s Empirical Rules which states that vibrational energy is more efficient at driving a reaction with a late transition state than translational energy. [2]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719938</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719938"/>
		<updated>2018-05-17T15:00:28Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.81 Å and BC was 0.75 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
This state that vibrational energy is more efficient in promoting a late-barrier reaction than translational energy&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719914</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719914"/>
		<updated>2018-05-17T14:58:37Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.81 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
This state that vibrational energy is more efficient in promoting a late-barrier reaction than translational energy&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719909</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719909"/>
		<updated>2018-05-17T14:58:14Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Polanyi&amp;#039;s rules */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
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From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
This state that vibrational energy is more efficient in promoting a late-barrier reaction than translational energy&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719906</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719906"/>
		<updated>2018-05-17T14:57:56Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Polanyi&amp;#039;s rules */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
 This state that vibrational energy is more efficient in promoting a late-barrier reaction than translational energy&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719834</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719834"/>
		<updated>2018-05-17T14:52:05Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719818</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719818"/>
		<updated>2018-05-17T14:51:15Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Locating the Transition State */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719815</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719815"/>
		<updated>2018-05-17T14:51:08Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Locating the Transition State */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719813</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719813"/>
		<updated>2018-05-17T14:51:00Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Locating the Transition State */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719810</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719810"/>
		<updated>2018-05-17T14:50:52Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Locating the Transition State */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 300px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 300px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719807</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719807"/>
		<updated>2018-05-17T14:50:39Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Locating the Transition State */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | centre | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719805</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719805"/>
		<updated>2018-05-17T14:50:26Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Locating the Transition State */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719803</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719803"/>
		<updated>2018-05-17T14:50:14Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Locating the Transition State */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
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From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719715</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719715"/>
		<updated>2018-05-17T14:42:42Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
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=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
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=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719713</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719713"/>
		<updated>2018-05-17T14:42:35Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719711</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719711"/>
		<updated>2018-05-17T14:42:28Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719709</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719709"/>
		<updated>2018-05-17T14:42:16Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the contour and momenta graphs, it can be seen the high level of vibrational energy, showing the energy released form the exothermic process is being transferred into kinetic vibrations. The energy plot clearly shows the conservation of energy, as the kinetic rises, the potential falls et vice versa.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719683</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719683"/>
		<updated>2018-05-17T14:38:43Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | centre | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719679</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719679"/>
		<updated>2018-05-17T14:38:25Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left | Reaction trajectory]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | right | Momentum vs Time]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left | Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719666</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719666"/>
		<updated>2018-05-17T14:36:59Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | right]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719662</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719662"/>
		<updated>2018-05-17T14:36:36Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | right]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719660</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719660"/>
		<updated>2018-05-17T14:36:17Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
From the graph it was seen the AB distance, for determining the trajectory, was 1.8 Å and BC was 0.78 Å, with momenta of -0.5 and 0.8 kg.m/sec respectively. The contour plot of which is shown:&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 FHreaction traj.PNG | thumb | 300px | left]]&lt;br /&gt;
[[File:HJW116 FHreaction momentavstime.PNG | thumb | 300px | right]]&lt;br /&gt;
[[File:HJW116 FHreaction energyvstime.PNG | thumb | 300px | left]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:HJW116_FHreaction_energyvstime.PNG&amp;diff=719659</id>
		<title>File:HJW116 FHreaction energyvstime.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:HJW116_FHreaction_energyvstime.PNG&amp;diff=719659"/>
		<updated>2018-05-17T14:36:06Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:HJW116_FHreaction_momentavstime.PNG&amp;diff=719654</id>
		<title>File:HJW116 FHreaction momentavstime.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:HJW116_FHreaction_momentavstime.PNG&amp;diff=719654"/>
		<updated>2018-05-17T14:35:33Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:HJW116_FHreaction_traj.PNG&amp;diff=719647</id>
		<title>File:HJW116 FHreaction traj.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:HJW116_FHreaction_traj.PNG&amp;diff=719647"/>
		<updated>2018-05-17T14:34:51Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719545</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719545"/>
		<updated>2018-05-17T14:26:17Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Activation Energy */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) graph the activation energy was seen to be to be 29.16 kcal/mol (121.99 kJ/mol).&lt;br /&gt;
&lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
==== Dynamics ====&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:sp2416&amp;diff=719526</id>
		<title>MRD:sp2416</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:sp2416&amp;diff=719526"/>
		<updated>2018-05-17T14:25:05Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* PES Inspection */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===Transition State ===&lt;br /&gt;
&lt;br /&gt;
The transition state is defined at the maximum on the minimum energy path linking reactants and products. Both minima and transition states are saddle points on the potential energy surface. On the potential energy surface diagram of H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; analysed, the gradient of both the transition state and minimum are found to be zero (∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0). Minima and transition structures can be distinguished by taking the second derivative of the gradient. For transition state this will be negative and positive, while for minima the answer to this will be positive.&lt;br /&gt;
&lt;br /&gt;
===Locating the Transition State===&lt;br /&gt;
&lt;br /&gt;
[[File:Internucleardistancesp2416.PNG|thumb|centre|Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
On the first graph the Transition state is where the A-B and B-C lines cross.&lt;br /&gt;
&lt;br /&gt;
To locate the Transition state the momenta are changed to 0, (as a transition state is a saddle point)  and then the distances AB and BC are adjusted so as to get an Internuclear Distance graph where both distances are stationary. This distance is found to be stationary when both AB and BC are set to be 0.90755.&lt;br /&gt;
&lt;br /&gt;
[[File:InternucleardistanceTSsp2416.PNG|thumb|centre|Internuclear Distance vs Time plot for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; Transition state]]&lt;br /&gt;
&lt;br /&gt;
===Dynamic and MEP Calculation types===&lt;br /&gt;
&lt;br /&gt;
The following results were obtained when the AB distance was changed to 0.90855 and the BC distance was maintained at 0.09755 (transition state position)&lt;br /&gt;
&lt;br /&gt;
[[File:Trajectory_plot_dynamics_sp2416.PNG|thumb|centre|Trajectory plot using Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:Trajectory_plot_mep_sp2416.PNG|thumb|centre|Trajectory plot using mep calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:Distance_time_dynamics_sp2416.PNG|thumb|centre|Internuclear Distance vs Time graph using Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:Distance_time_mep_sp2416.PNG|thumb|centre|Internuclear Distance vs Time graph using mep calculation type]]&lt;br /&gt;
&lt;br /&gt;
===Reactive and Unreactive Trajectories===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of different momenta on reactivity (Dynamic Calculation Type)&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Total Energy!!Type of Trajectory!!Contour plot!!Description&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:Contour1_sp2416.PNG|320px]] ||The reaction starts with a minorly oscillating AB-molecule, which is shown by a straight line plot at the start. Post the transition state occurring, and the BC-bond has been formed the molecule starts oscillating stronger. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Uneactive || [[File:Contour2_sp2416.PNG|320px]] || The A-B bond is oscillating at the beginning. However, both momenta of AB and C together are not strong enough to overcome the repulsion force and build the BC molecule. The particles however do approach each other, but the reaction does not go to completion. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:Contour3_sp2416.PNG|320px]] || Very similar to the first reaction, the only difference being that the A-B bond oscillates from the beginning as C is approaching.||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:Contour4_sp2416.PNG|320px]] || The A-B bond does not oscillate. The impact with atom C leads to a brief period of time where B and C can be observed vibrating strongly, before it dissociates again.||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:Contour5_sp2416.PNG|320px]] || This plot can be considered as the mirror image of the previous plot as it starts with a non-oscillating A-B bond. Collision with C give a short-lived BC bond, which dissociates back to A-B. However, the reaction goes back to a B-C molecule.&lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Transition State Theory===&lt;br /&gt;
&lt;br /&gt;
Transition State theory separates reaction systems into the reactant-space and the product-space region. In the reactant-space the starting material has not reacted yet and the product-space region is entered after the reaction occurs. The border between these two systems is defined as the transition state. As soon as the transition state is overcomed and the products are produced, the reaction cannot be reveresed and the reactant-space cannot be entered again.&lt;br /&gt;
&lt;br /&gt;
The theory assumes that the atoms obey the Born-Oppenheimer approximation and that quantum-tunneling effects do not occur. Also, the atoms of the starting material obey the Boltzmann Distribution and hence we assume that the system has enough time to equilibrate at the beginning. &lt;br /&gt;
&lt;br /&gt;
However, upon consideration of the above calculations for the 4th reaction, it can be observed that the reactants are actually able to enter the product space and dissociate back to the starting material. Hence the theory cannot be applied here. The reason for this is because the calculations performed by the program are assuming isolation of the reactant system, while the theory takes the surrounding and the possible energy exchange with neighbouring molecules into account, in order to achieve equilibrium.&lt;br /&gt;
&lt;br /&gt;
==F - H - H ==&lt;br /&gt;
&lt;br /&gt;
=== PES Inspection ===&lt;br /&gt;
&lt;br /&gt;
The equilibrium reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF is exothermic when it goes forward releasing energy, whilst the backward reaction is endothermic, taking energy in. &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt; The H-H bond is -432 kJ/mol and the H-F bond is -565 kj/mol &amp;lt;ref name=&amp;quot;[2]&amp;quot; /&amp;gt;. This means that more energy is needed to break the H-F than the energy gained by forming the H-H bond, and hence the forward reaction is exothermic (and the backward endothermic).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Locating the Transition Stateː &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Applying the following settingsː&lt;br /&gt;
&lt;br /&gt;
Atom A: F &lt;br /&gt;
&lt;br /&gt;
Atom B: H &lt;br /&gt;
&lt;br /&gt;
Atom C: H&lt;br /&gt;
&lt;br /&gt;
AB distance: 1.81 Å&lt;br /&gt;
&lt;br /&gt;
BC distance: 0.7455 Å&lt;br /&gt;
&lt;br /&gt;
Both momenta are set to 0.&lt;br /&gt;
&lt;br /&gt;
These settings were applied using the Dynamics Calculation type and visualising the Internuclear Distance vs Time plot. Trial and error values were used until all the distances (A-B, B-C and A-C) produce straight lines, as shown in the figure below.&lt;br /&gt;
&lt;br /&gt;
[[File:Distance_time_1_sp2416.PNG|thumb|centre|Internuclear Distance vs Time graph using Dynamics calculation type for F-H-H]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt; Reporting the Activation Energyː &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To find the activation energy, the type of calculation used is MEP and the AB distance is displaced slightly (form 1.81 is changed to 1.83) in order to force the reaction to go to either direction of the equilibrium - right hand side or left hand side. &lt;br /&gt;
&lt;br /&gt;
The forward reaction in the equilibrium F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF is exothermic. Hammond&#039;s postulate states that the transition state resembles more the reactants than the products in an exothermic reaction. Hence, the activation energy is obtained when the A-B distance is displaced in this calculation.&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
Energy of the transition state = -103.752 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Energy of products = -133.466 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Activation energy of the reaction = 29.714 cal/mol&lt;br /&gt;
&lt;br /&gt;
[[File:Activationenergysp2416.PNG|thumb|centre|Finding the activation energy]]&lt;br /&gt;
&lt;br /&gt;
=== Reaction Dynamics ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Reactive Trajectory &amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Atom A : F &lt;br /&gt;
&lt;br /&gt;
Atom B : H &lt;br /&gt;
&lt;br /&gt;
Atom C : H &lt;br /&gt;
&lt;br /&gt;
AB distance = 1.91 Å&lt;br /&gt;
&lt;br /&gt;
BC distance = 0.7455 Å&lt;br /&gt;
&lt;br /&gt;
AB momentum = -1.5 &lt;br /&gt;
&lt;br /&gt;
BC momentum = 1.0&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Reactivetrajsp2416.png|thumb|centre|Reactive Trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Momentasp2416.png|thumb|centre|Internuclear Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
An increased and vigorous oscillation of the resulting molecule can be seen from the Momentum vs Time plot. This means that the energy released during this exothermic reaction is converted into vibrational energy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Energyplotsp2416.png|thumb|centre|Energy vs Time]]&lt;br /&gt;
&lt;br /&gt;
The Energy vs Time plot shows an increased oscillation in the kinetic energy of the molecule.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Investigating the effect of changing the momentum of AB&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Atom A : F &lt;br /&gt;
&lt;br /&gt;
Atom B : H &lt;br /&gt;
&lt;br /&gt;
Atom C : H&lt;br /&gt;
&lt;br /&gt;
AB distance = 1.91 Å&lt;br /&gt;
&lt;br /&gt;
BC distance = 0.7455 Å&lt;br /&gt;
&lt;br /&gt;
AB momentum = -3 to 3 &lt;br /&gt;
&lt;br /&gt;
BC momentum = -0.5&lt;br /&gt;
&lt;br /&gt;
=== Polanyi&#039;s rules ===&lt;br /&gt;
&lt;br /&gt;
The different motions (e.g. vibrational and rotational) on a reaction are discussed by Polanyi Rules. &lt;br /&gt;
&lt;br /&gt;
As the forward reaction in  F + H2 ⇌ H + HF  is exothermic, the transition state resembles the reactants and occurs early, and therefore is promoted by translational motion. This motion is resembled by the momentum corresponding to the molecules which initially are further apart (in this case the AB momentum), as this momentum is responsible for the strength of the collision.&lt;br /&gt;
&lt;br /&gt;
In the backward reaction which is endothermic, the transition state is late and is hence promoted by a high initial vibrational energy of the starting material. The momentum of the initially bonded molecule represents this energy. &lt;br /&gt;
&lt;br /&gt;
Thus, it depends on the reaction monitored which momentum leads to a promotion of which reaction.&lt;br /&gt;
&lt;br /&gt;
The reaction examined above corresponds to the endothermic one, which explains why an increase in the AB-momentum results in no reaction.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;J.C. Polanyi, D.C. Tardy, 1969, J. Chem. Phys., Vol.51 &amp;quot;Energy Distribution in the Exothermic Reaction F + H2 , and the Endothermic Reaction HF + H&amp;quot;, p.255-321.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[2]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 15/05/2018 17ː10).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719441</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719441"/>
		<updated>2018-05-17T14:15:22Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) &lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719440</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719440"/>
		<updated>2018-05-17T14:15:10Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Activation Energy */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.91 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) &lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719433</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719433"/>
		<updated>2018-05-17T14:14:44Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Activation Energy */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.83 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) &lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px |  MEP Energy vs time]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719417</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719417"/>
		<updated>2018-05-17T14:13:21Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Exercise 2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph of IN distance vs Time (derivative = 0). Through trial and error, this gave values of AB=1.812 Å and BC=0.745 Å in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.) This gave a straight line graph, thus showing the correct value had been obtained.&lt;br /&gt;
&lt;br /&gt;
=== Activation Energy ===&lt;br /&gt;
&lt;br /&gt;
By slight alteration of the equilibrium settings (AB being changed to 1.83 Å) we can force the reaction to one side. In this case, due to the extended bond length, towards the F  + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; side.&lt;br /&gt;
&lt;br /&gt;
Using an MEP (Energy vs Time) &lt;br /&gt;
[[File:H2 F energydiagram.PNG| thumb | left | 320px]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:H2_F_energydiagram.PNG&amp;diff=719409</id>
		<title>File:H2 F energydiagram.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:H2_F_energydiagram.PNG&amp;diff=719409"/>
		<updated>2018-05-17T14:11:53Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719298</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=719298"/>
		<updated>2018-05-17T13:57:50Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Exercise 2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken. This can be attributed due to the increased ionic character between the F-H bond due to the change in electronegativity. The reverse direction is therefore endothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In order to determine the transition state the saddle state was needed. This was, again, determined via the maximum of an MEP graph (dervitive = 0). Through trial and error, this gave values of AB=1.812 a.u. and BC=0.745 a.u. in which A is Flourine, and B,C are both Hydrogen. (Momenta was set to zero.)&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=717893</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=717893"/>
		<updated>2018-05-16T17:55:26Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Exercise 1 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=717892</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=717892"/>
		<updated>2018-05-16T17:55:03Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Exercise 1 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=717890</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=717890"/>
		<updated>2018-05-16T17:53:47Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 16/05/2018 18ː53).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=717887</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=717887"/>
		<updated>2018-05-16T17:51:06Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* References = */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 15/05/2018 17ː10).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=717886</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=717886"/>
		<updated>2018-05-16T17:50:58Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* References = */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 15/05/2018 17ː10).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=717885</id>
		<title>MRD:HJW116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:HJW116&amp;diff=717885"/>
		<updated>2018-05-16T17:50:20Z</updated>

		<summary type="html">&lt;p&gt;Hjw116: /* Exercise 2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1 ==&lt;br /&gt;
&lt;br /&gt;
=== Transition state ===&lt;br /&gt;
&lt;br /&gt;
A potential energy surface graph is gained from a function with two variables, in this case distance of AB, and BC. The transition state is seen at &amp;quot;saddle points&amp;quot; on the plotted graph. These are the maxima and minimas of the energy plot. These occur when the derivatives of each variable is equal to 0.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
To determine whether it is a maxima or minima, take the double derivative; a positive value gives a minima, and negative, the maxima.&lt;br /&gt;
&lt;br /&gt;
=== Locating the Transition State ===&lt;br /&gt;
&lt;br /&gt;
[[File:HJW Transition state H2+H.png | thumb | left | 200px | The point where the line AB and BC cross gives the value for the first transition state.]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW starightline TSthing.png | thumb | right | 200px | The initial momentum has been set to zero, in order for there not to be enough energy to escape the potential well.]]&lt;br /&gt;
&lt;br /&gt;
In order to maintain a set distance over time, AB and BC were made equal and set to a variety of values; 0.908 giving a straight line (non-changing distance)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== MEP and Dynamic Calculations ===&lt;br /&gt;
&lt;br /&gt;
The plot of the MEP follows the lowest energy path for the reaction, where the velocity of the molecule is continuously returned to 0 as to remove inertia from making any effect. This is seen on the MEP plot, not the dynamic.&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn cont H2.png | thumb | left | Trajectory plot-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP cont H2.png | thumb | centre | Trajectory plot-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 Dyn dis-time H2.png | thumb | left | Distance vs Time graph-Dynamics calculation type]]&lt;br /&gt;
&lt;br /&gt;
[[File:HJW116 MEP dis-time H2.png | thumb | centre | Distance vs Time graph-MEP calculation type]]&lt;br /&gt;
&lt;br /&gt;
=== Reactive and Unreactive Trajectories ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Effect of inertia (Dynamic calculation type)&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;sup&amp;gt;Total&amp;lt;/sup&amp;gt; !! React/Non!!Contour plot !! Discussion &lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || -99.199 || Reactive || [[File:HJW SP react1b.PNG|315px]] ||Prior to the transition state, the AB molecule does not oscillate (shown by the straight line) Once the minima has been passed, and the BC bond is formed, the bond starts oscillating more. ||&lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.0 || -100.456 || Unreactive || [[File:HJW SP react2.PNG|315px]] || Despite the bond approaching each other at the start, the momentum of each (AB and C) are not strong enough to overcome the repulsive forces involved.  &lt;br /&gt;
|-&lt;br /&gt;
| -1.5 || -2.5 || -98.956 || Reactive || [[File:HJW SP react3.PNG|315px]] || Simple reaction, AB approach C, whilst vibrating, where BC forms and the strength of vibration continues.&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.0 || -84.956 || Uneactive || [[File:HJW SP react4.PNG|315px]] || There is no oscillation at the start whereas, upon contact with C, there is a period of heavy vibrations, that leads to dissociation of the molecule.  .||&lt;br /&gt;
|-&lt;br /&gt;
| -2.5 || -5.2 || -83.416 || Reactive || [[File:HJW SP react5.PNG|315px]] || In a similar way to the reaction above, this gives, upon collision of AB and C, a short lived BC bond that quickly dissociates. However, the reaction continues and a BC molecule is successfully created with strong oscillation. &lt;br /&gt;
||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Transition state theory ===&lt;br /&gt;
&lt;br /&gt;
A key point to the theory is that the atoms follow the Born-Oppenheimer approximation and ignores the effects of quantum tunneling. It is also assumed that the starting products are equlibrating as according to the energies given by the Boltzmann Distribution. The theory also separates the products and reactants into separate &amp;quot;spaces&amp;quot; with the transition being the middle point of this, where the theoretical product is a mix of the two. Once the state has collapsed and the product is formed, the reaction is irreversible under the same conditions.&lt;br /&gt;
&lt;br /&gt;
My 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; and 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; reaction however, shows the making of product, followed by the state transition back to reactants. Thus breaking the theory. This could be attributed to the calculation being run assuming an isolated system, where as the theory accounts for the external factors as well to determine the equilibrium.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Exercise 2 ==&lt;br /&gt;
&lt;br /&gt;
As the H-H bond is (-432 kJ/mol), and the F-H is higher in energy (-565 kJ/mol) &amp;lt;ref name=&amp;quot;[1]&amp;quot; /&amp;gt;, the reaction (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ⇌ H + HF) is, therefore exothermic, as the energy released from the making of the H-F bond is greater than that taken from the H-H being broken.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;ref name=&amp;quot;[1]&amp;quot;&amp;gt;http://www.wiredchemist.com/chemistry/data/bond_energies_lengths.html (Assessed on 15/05/2018 17ː10).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Hjw116</name></author>
	</entry>
</feed>