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	<id>https://chemwiki.ch.ic.ac.uk/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=Mhz15</id>
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	<updated>2026-04-05T18:35:54Z</updated>
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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615483</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615483"/>
		<updated>2017-05-05T15:45:05Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn.png|center]]&lt;br /&gt;
&lt;br /&gt;
The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Surface plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_potential_energy_surface.png|center|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The surface plot shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
&lt;br /&gt;
The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
&lt;br /&gt;
The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Interpreting the distance vs time plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_transition_state_distance_-_LABELLED.png|center|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The sequence shown illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_(ed)_distance_vs_time.png|center|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
&lt;br /&gt;
The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
&lt;br /&gt;
The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|center|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The plot illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
 &lt;br /&gt;
The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Reaction path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
&lt;br /&gt;
The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Reactive and unreactive trajectories&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
Trajectories with the following momenta combination were run while p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Reactivity&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || Unreactive&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || Unreactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || Unreactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || Reactive&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
[[File:1.png|center|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
&lt;br /&gt;
The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
&lt;br /&gt;
This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:2.png|center|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
&lt;br /&gt;
The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
&lt;br /&gt;
The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
&lt;br /&gt;
[[File:3.png|center|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
&lt;br /&gt;
The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
&lt;br /&gt;
This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
&lt;br /&gt;
[[File:4.png|center|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
&lt;br /&gt;
The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
&lt;br /&gt;
H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
&lt;br /&gt;
The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
&lt;br /&gt;
[[File:5.png|center|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
&lt;br /&gt;
The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
&lt;br /&gt;
This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Classifying endothermic and exothermic reactions&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
In the H + HF reaction, the bond breaking is between the hydrogen and fluorine atoms. The H-F bond is relatively stronger due to a large difference of electronegativities between that of hyrodgen and fluorine atoms. Fluorine attracts the hydrogen atom stronger. Thus a large amount of energy is required to break the bond, and this makes the H + HF reaction endothermic.&lt;br /&gt;
&lt;br /&gt;
In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the bond breaking is between the two hydrogen atoms. The H-H bond is relatively weaker due to an approximately zero difference of electronegativities between the two atoms. A smaller amount of energy is required to break the H-H bond, thus the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;The transition state&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:Ts_estimation_distance-time.png|center|thumb|325x325px|The internuclear distance vs time plot at which the transition state occurs.]]&lt;br /&gt;
&lt;br /&gt;
The plot on the center illustrates the transition state of an F - H - H reaction, and it occurs when r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.811 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.744 Å, and the initial momenta set to 0.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Activation energies&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:EA_hh_%2B_f.png|center|thumb|325x325px|The surface plot showing the saddle point in the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.]]&lt;br /&gt;
&lt;br /&gt;
In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the transition state resembles the reactants more due to its exothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the reactants is equal to the activation energy. The activation energy is found to be 22.574 kcal/mol.&lt;br /&gt;
&lt;br /&gt;
[[File:EA_hf_%2B_h.png|center|thumb|325x325px|The surface plot showing the saddle point in the H + HF reaction.]]&lt;br /&gt;
&lt;br /&gt;
In the H + HF reaction, the transition state resembles the products more due to its endothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the products is equal to the activation energy. The activation energy was found to be 28 kcal/mol.&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Reaction dynamics&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
==== &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction&#039;&#039;&#039; ====&lt;br /&gt;
&lt;br /&gt;
[[File:Reactive_trajectory.png|center|thumb|325x325px|The surface plot showing an example of a reactive trajectory.]]&lt;br /&gt;
&lt;br /&gt;
The reactive trajectory was found using initial conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.48 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74 Å, while momenta were set to 0.&lt;br /&gt;
&lt;br /&gt;
As F approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and forms a bond with the atom, its potential energy increases, and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, the leaving atom, loses potential energy and gains kinetic energy.&lt;br /&gt;
&lt;br /&gt;
===== &#039;&#039;&#039;Testing different p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; values&#039;&#039;&#039; =====&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Idek.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -3.0.]]&lt;br /&gt;
| [[File:Idek1.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = - 2.0.]]&lt;br /&gt;
| [[File:Idek2.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -1.0.]]&lt;br /&gt;
|}&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Idek3.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 1.0.]]&lt;br /&gt;
| [[File:Idek4.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0.]]&lt;br /&gt;
| [[File:Idek5.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 3.0.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
A range of values for p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; from -3.0 to 3.0 was explored with the trajectory starting at the bottom of the well. The conditions used were r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.48 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74 Å and p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.5. In all of the reactions tested, the products are converted back to the reactants. This is due to there being an excessive amount of energy into the system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Idk1.png|center|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.8 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.1.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Using the same initial conditions as above, the reaction was tested with p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.8 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.1, reducing the overall energy of the system.&lt;br /&gt;
&lt;br /&gt;
The trajectory leads to a reaction but H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and F remain in oscillation relative to the central H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== &#039;&#039;&#039;H + HF reaction&#039;&#039;&#039; ====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Hp1.png|center|thumb|275x275px|The trajectory when r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 1.811 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74 Å and p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.2, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -2.2.]]&lt;br /&gt;
&lt;br /&gt;
The value of p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; was set to a high value above the activation energy.&lt;br /&gt;
&lt;br /&gt;
[[File:Hp2.png|center|thumb|275x275px|The trajectory with the same conditions as above except p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -1.2.]]&lt;br /&gt;
&lt;br /&gt;
The trajectory leads to a reaction when p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -1.2.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615477</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615477"/>
		<updated>2017-05-05T15:44:19Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|center|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|center|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|center|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|center|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
 &lt;br /&gt;
The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
|}&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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Trajectories with the following momenta combination were run while p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Reactivity&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || Reactive&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0 || Unreactive&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5 || Unreactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0 || Unreactive&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2 || Reactive&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
[[File:1.png|center|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|center|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|center|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|center|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|center|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
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== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;br /&gt;
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=== &#039;&#039;&#039;Classifying endothermic and exothermic reactions&#039;&#039;&#039; ===&lt;br /&gt;
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In the H + HF reaction, the bond breaking is between the hydrogen and fluorine atoms. The H-F bond is relatively stronger due to a large difference of electronegativities between that of hyrodgen and fluorine atoms. Fluorine attracts the hydrogen atom stronger. Thus a large amount of energy is required to break the bond, and this makes the H + HF reaction endothermic.&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the bond breaking is between the two hydrogen atoms. The H-H bond is relatively weaker due to an approximately zero difference of electronegativities between the two atoms. A smaller amount of energy is required to break the H-H bond, thus the reaction is exothermic.&lt;br /&gt;
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=== &#039;&#039;&#039;The transition state&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Ts_estimation_distance-time.png|center|thumb|325x325px|The internuclear distance vs time plot at which the transition state occurs.]]&lt;br /&gt;
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The plot on the center illustrates the transition state of an F - H - H reaction, and it occurs when r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.811 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.744 Å, and the initial momenta set to 0.&lt;br /&gt;
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=== &#039;&#039;&#039;Activation energies&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:EA_hh_%2B_f.png|center|thumb|325x325px|The surface plot showing the saddle point in the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.]]&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the transition state resembles the reactants more due to its exothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the reactants is equal to the activation energy. The activation energy is found to be 22.574 kcal/mol.&lt;br /&gt;
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[[File:EA_hf_%2B_h.png|center|thumb|325x325px|The surface plot showing the saddle point in the H + HF reaction.]]&lt;br /&gt;
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In the H + HF reaction, the transition state resembles the products more due to its endothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the products is equal to the activation energy. The activation energy was found to be 28 kcal/mol.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction dynamics&#039;&#039;&#039; ===&lt;br /&gt;
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==== &#039;&#039;&#039;F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction&#039;&#039;&#039; ====&lt;br /&gt;
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[[File:Reactive_trajectory.png|center|thumb|325x325px|The surface plot showing an example of a reactive trajectory.]]&lt;br /&gt;
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The reactive trajectory was found using initial conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.48 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74 Å, while momenta were set to 0.&lt;br /&gt;
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As F approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and forms a bond with the atom, its potential energy increases, and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, the leaving atom, loses potential energy and gains kinetic energy.&lt;br /&gt;
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===== &#039;&#039;&#039;Testing different p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; values&#039;&#039;&#039; =====&lt;br /&gt;
&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Idek.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -3.0.]]&lt;br /&gt;
| [[File:Idek1.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = - 2.0.]]&lt;br /&gt;
| [[File:Idek2.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -1.0.]]&lt;br /&gt;
|}&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Idek3.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 1.0.]]&lt;br /&gt;
| [[File:Idek4.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0.]]&lt;br /&gt;
| [[File:Idek5.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 3.0.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
A range of values for p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; from -3.0 to 3.0 was explored with the trajectory starting at the bottom of the well. The conditions used were r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.48 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74 Å and p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.5. In all of the reactions tested, the products are converted back to the reactants. This is due to there being an excessive amount of energy into the system.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Idk1.png|center|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.8 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.1.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Using the same initial conditions as above, the reaction was tested with p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.8 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.1, reducing the overall energy of the system.&lt;br /&gt;
&lt;br /&gt;
The trajectory leads to a reaction but H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and F remain in oscillation relative to the central H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== &#039;&#039;&#039;H + HF reaction&#039;&#039;&#039; ====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Hp1.png|center|thumb|275x275px|The trajectory when r&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = 1.811 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74 Å and p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.2, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -2.2.]]&lt;br /&gt;
&lt;br /&gt;
The value of p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; was set to a high value above the activation energy.&lt;br /&gt;
&lt;br /&gt;
[[File:Hp2.png|center|thumb|275x275px|The trajectory with the same conditions as above except p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -1.2.]]&lt;br /&gt;
&lt;br /&gt;
The trajectory leads to a reaction when p&amp;lt;sub&amp;gt;HF&amp;lt;/sub&amp;gt; = -0.1 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -1.2.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hp2.png&amp;diff=615440</id>
		<title>File:Hp2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hp2.png&amp;diff=615440"/>
		<updated>2017-05-05T15:34:07Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hp1.png&amp;diff=615405</id>
		<title>File:Hp1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hp1.png&amp;diff=615405"/>
		<updated>2017-05-05T15:22:41Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
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&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615355</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615355"/>
		<updated>2017-05-05T15:11:09Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* Testing different pHH and pFH values */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
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== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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Trajectories with the following momenta combination were run while p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Reactivity&lt;br /&gt;
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| -1.25 || -2.5 || Reactive&lt;br /&gt;
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| -1.5  || -2.5 || Unreactive&lt;br /&gt;
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| -2.5  || -5.0 || Unreactive&lt;br /&gt;
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| -2.5  || -5.2 || Reactive&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
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== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;br /&gt;
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=== &#039;&#039;&#039;Classifying endothermic and exothermic reactions&#039;&#039;&#039; ===&lt;br /&gt;
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In the H + HF reaction, the bond breaking is between the hydrogen and fluorine atoms. The H-F bond is relatively stronger due to a large difference of electronegativities between that of hyrodgen and fluorine atoms. Fluorine attracts the hydrogen atom stronger. Thus a large amount of energy is required to break the bond, and this makes the H + HF reaction endothermic.&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the bond breaking is between the two hydrogen atoms. The H-H bond is relatively weaker due to an approximately zero difference of electronegativities between the two atoms. A smaller amount of energy is required to break the H-H bond, thus the reaction is exothermic.&lt;br /&gt;
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=== &#039;&#039;&#039;The transition state&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Ts_estimation_distance-time.png|left|thumb|325x325px|The internuclear distance vs time plot at which the transition state occurs.]]&lt;br /&gt;
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The plot on the left illustrates the transition state of an F - H - H reaction, and it occurs when r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.811 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.744 Å, and the initial momenta set to 0.&lt;br /&gt;
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=== &#039;&#039;&#039;Activation energies&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:EA_hh_%2B_f.png|left|thumb|325x325px|The surface plot showing the saddle point in the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.]]&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the transition state resembles the reactants more due to its exothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the reactants is equal to the activation energy. The activation energy is found to be 22.574 kcal/mol.&lt;br /&gt;
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[[File:EA_hf_%2B_h.png|left|thumb|325x325px|The surface plot showing the saddle point in the H + HF reaction.]]&lt;br /&gt;
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In the H + HF reaction, the transition state resembles the products more due to its endothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the products is equal to the activation energy. The activation energy was found to be 28 kcal/mol.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction dynamics&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Reactive_trajectory.png|left|thumb|325x325px|The surface plot showing an example of a reactive trajectory.]]&lt;br /&gt;
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The reactive trajectory was found using initial conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.48 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74 Å, while momenta were set to 0.&lt;br /&gt;
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As F approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and forms a bond with the atom, its potential energy increases, and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, the leaving atom, loses potential energy and gains kinetic energy.&lt;br /&gt;
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=== &#039;&#039;&#039;Testing different p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; values&#039;&#039;&#039; ===&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Idek.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -3.0.]]&lt;br /&gt;
| [[File:Idek1.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = - 2.0.]]&lt;br /&gt;
| [[File:Idek2.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -1.0.]]&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Idek3.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 1.0.]]&lt;br /&gt;
| [[File:Idek4.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0.]]&lt;br /&gt;
| [[File:Idek5.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 3.0.]]&lt;br /&gt;
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A range of values for p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; from -3.0 to 3.0 was explored with the trajectory starting at the bottom of the well. The conditions used were r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.48 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74 Å and p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.5. In all of the reactions tested, the products are converted back to the reactants. This is due to there being an excessive amount of energy into the system.&lt;br /&gt;
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[[File:Idk1.png|left|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.8 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.1.]]&lt;br /&gt;
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Using the same initial conditions as above, the reaction was tested with p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.8 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.1, reducing the overall energy of the system.&lt;br /&gt;
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The trajectory leads to a reaction but H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and F remain in oscillation relative to the central H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615348</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615348"/>
		<updated>2017-05-05T15:09:12Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* Reaction dynamics */&lt;/p&gt;
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&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
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This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
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== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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Trajectories with the following momenta combination were run while p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Reactivity&lt;br /&gt;
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| -1.25 || -2.5 || Reactive&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
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== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;br /&gt;
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=== &#039;&#039;&#039;Classifying endothermic and exothermic reactions&#039;&#039;&#039; ===&lt;br /&gt;
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In the H + HF reaction, the bond breaking is between the hydrogen and fluorine atoms. The H-F bond is relatively stronger due to a large difference of electronegativities between that of hyrodgen and fluorine atoms. Fluorine attracts the hydrogen atom stronger. Thus a large amount of energy is required to break the bond, and this makes the H + HF reaction endothermic.&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the bond breaking is between the two hydrogen atoms. The H-H bond is relatively weaker due to an approximately zero difference of electronegativities between the two atoms. A smaller amount of energy is required to break the H-H bond, thus the reaction is exothermic.&lt;br /&gt;
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=== &#039;&#039;&#039;The transition state&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Ts_estimation_distance-time.png|left|thumb|325x325px|The internuclear distance vs time plot at which the transition state occurs.]]&lt;br /&gt;
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The plot on the left illustrates the transition state of an F - H - H reaction, and it occurs when r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.811 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.744 Å, and the initial momenta set to 0.&lt;br /&gt;
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=== &#039;&#039;&#039;Activation energies&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:EA_hh_%2B_f.png|left|thumb|325x325px|The surface plot showing the saddle point in the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.]]&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the transition state resembles the reactants more due to its exothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the reactants is equal to the activation energy. The activation energy is found to be 22.574 kcal/mol.&lt;br /&gt;
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[[File:EA_hf_%2B_h.png|left|thumb|325x325px|The surface plot showing the saddle point in the H + HF reaction.]]&lt;br /&gt;
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In the H + HF reaction, the transition state resembles the products more due to its endothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the products is equal to the activation energy. The activation energy was found to be 28 kcal/mol.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction dynamics&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Reactive_trajectory.png|left|thumb|325x325px|The surface plot showing an example of a reactive trajectory.]]&lt;br /&gt;
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The reactive trajectory was found using initial conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.48 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74 Å, while momenta were set to 0.&lt;br /&gt;
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As F approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and forms a bond with the atom, its potential energy increases, and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, the leaving atom, loses potential energy and gains kinetic energy.&lt;br /&gt;
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=== &#039;&#039;&#039;Testing different p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; values&#039;&#039;&#039; ===&lt;br /&gt;
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{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Idek.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -3.0.]]&lt;br /&gt;
| [[File:Idek1.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = - 2.0.]]&lt;br /&gt;
| [[File:Idek2.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -1.0.]]&lt;br /&gt;
|}&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Idek3.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 1.0.]]&lt;br /&gt;
| [[File:Idek4.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 2.0.]]&lt;br /&gt;
| [[File:Idek5.png|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 3.0.]]&lt;br /&gt;
|}&lt;br /&gt;
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A range of values for p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; from -3.0 to 3.0 was explored with the trajectory starting at the bottom of the well. The conditions used were r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.48 Å, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74 Å and p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.5. In all of the reactions tested, the products are converted back to the reactants. This is due to there being an excessive amount of energy into the system.&lt;br /&gt;
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[[File:Idk1.png|left|thumb|275x275px|The trajectory when p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.8 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.1.]]&lt;br /&gt;
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Using the same initial conditions as above, the reaction was tested with p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = -0.8 and p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.1, reducing the overall energy of the system.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idk1.png&amp;diff=615339</id>
		<title>File:Idk1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idk1.png&amp;diff=615339"/>
		<updated>2017-05-05T15:05:04Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
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&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idek5.png&amp;diff=615325</id>
		<title>File:Idek5.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idek5.png&amp;diff=615325"/>
		<updated>2017-05-05T14:56:27Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idek4.png&amp;diff=615323</id>
		<title>File:Idek4.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idek4.png&amp;diff=615323"/>
		<updated>2017-05-05T14:55:43Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idek3.png&amp;diff=615320</id>
		<title>File:Idek3.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idek3.png&amp;diff=615320"/>
		<updated>2017-05-05T14:54:54Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idek2.png&amp;diff=615316</id>
		<title>File:Idek2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idek2.png&amp;diff=615316"/>
		<updated>2017-05-05T14:53:55Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idek1.png&amp;diff=615313</id>
		<title>File:Idek1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idek1.png&amp;diff=615313"/>
		<updated>2017-05-05T14:53:05Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615302</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615302"/>
		<updated>2017-05-05T14:51:30Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* Reaction dynamics */&lt;/p&gt;
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&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
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This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
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== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
|}&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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Trajectories with the following momenta combination were run while p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Reactivity&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5 || Reactive&lt;br /&gt;
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| -1.5  || -2.0 || Unreactive&lt;br /&gt;
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| -1.5  || -2.5 || Unreactive&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
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== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;br /&gt;
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=== &#039;&#039;&#039;Classifying endothermic and exothermic reactions&#039;&#039;&#039; ===&lt;br /&gt;
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In the H + HF reaction, the bond breaking is between the hydrogen and fluorine atoms. The H-F bond is relatively stronger due to a large difference of electronegativities between that of hyrodgen and fluorine atoms. Fluorine attracts the hydrogen atom stronger. Thus a large amount of energy is required to break the bond, and this makes the H + HF reaction endothermic.&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the bond breaking is between the two hydrogen atoms. The H-H bond is relatively weaker due to an approximately zero difference of electronegativities between the two atoms. A smaller amount of energy is required to break the H-H bond, thus the reaction is exothermic.&lt;br /&gt;
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=== &#039;&#039;&#039;The transition state&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Ts_estimation_distance-time.png|left|thumb|325x325px|The internuclear distance vs time plot at which the transition state occurs.]]&lt;br /&gt;
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The plot on the left illustrates the transition state of an F - H - H reaction, and it occurs when r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.811 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.744 Å, and the initial momenta set to 0.&lt;br /&gt;
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=== &#039;&#039;&#039;Activation energies&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:EA_hh_%2B_f.png|left|thumb|325x325px|The surface plot showing the saddle point in the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.]]&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the transition state resembles the reactants more due to its exothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the reactants is equal to the activation energy. The activation energy is found to be 22.574 kcal/mol.&lt;br /&gt;
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[[File:EA_hf_%2B_h.png|left|thumb|325x325px|The surface plot showing the saddle point in the H + HF reaction.]]&lt;br /&gt;
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In the H + HF reaction, the transition state resembles the products more due to its endothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the products is equal to the activation energy. The activation energy was found to be 28 kcal/mol.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction dynamics&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Reactive_trajectory.png|left|thumb|325x325px|The surface plot showing an example of a reactive trajectory.]]&lt;br /&gt;
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The reactive trajectory was found using initial conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.48 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74 Å, while momenta were set to 0.&lt;br /&gt;
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As F approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and forms a bond with the atom, its potential energy increases, and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, the leaving atom, loses potential energy and gains kinetic energy.&lt;br /&gt;
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[[File:Idek.png|left|thumb|325x325px|The surface plot showing the trajectory when p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = -3.0.]]&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idek.png&amp;diff=615298</id>
		<title>File:Idek.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Idek.png&amp;diff=615298"/>
		<updated>2017-05-05T14:49:56Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615289</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615289"/>
		<updated>2017-05-05T14:48:05Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* F - H - H System */&lt;/p&gt;
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&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
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This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
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== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
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| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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Trajectories with the following momenta combination were run while p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Reactivity&lt;br /&gt;
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| -1.25 || -2.5 || Reactive&lt;br /&gt;
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| -2.5  || -5.0 || Unreactive&lt;br /&gt;
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| -2.5  || -5.2 || Reactive&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
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== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;br /&gt;
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=== &#039;&#039;&#039;Classifying endothermic and exothermic reactions&#039;&#039;&#039; ===&lt;br /&gt;
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In the H + HF reaction, the bond breaking is between the hydrogen and fluorine atoms. The H-F bond is relatively stronger due to a large difference of electronegativities between that of hyrodgen and fluorine atoms. Fluorine attracts the hydrogen atom stronger. Thus a large amount of energy is required to break the bond, and this makes the H + HF reaction endothermic.&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the bond breaking is between the two hydrogen atoms. The H-H bond is relatively weaker due to an approximately zero difference of electronegativities between the two atoms. A smaller amount of energy is required to break the H-H bond, thus the reaction is exothermic.&lt;br /&gt;
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=== &#039;&#039;&#039;The transition state&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Ts_estimation_distance-time.png|left|thumb|325x325px|The internuclear distance vs time plot at which the transition state occurs.]]&lt;br /&gt;
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The plot on the left illustrates the transition state of an F - H - H reaction, and it occurs when r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.811 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.744 Å, and the initial momenta set to 0.&lt;br /&gt;
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=== &#039;&#039;&#039;Activation energies&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:EA_hh_%2B_f.png|left|thumb|325x325px|The surface plot showing the saddle point in the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.]]&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the transition state resembles the reactants more due to its exothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the reactants is equal to the activation energy. The activation energy is found to be 22.574 kcal/mol.&lt;br /&gt;
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[[File:EA_hf_%2B_h.png|left|thumb|325x325px|The surface plot showing the saddle point in the H + HF reaction.]]&lt;br /&gt;
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In the H + HF reaction, the transition state resembles the products more due to its endothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the products is equal to the activation energy. The activation energy was found to be 28 kcal/mol.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction dynamics&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Reactive_trajectory.png|left|thumb|325x325px|The surface plot showing an example of a reactive trajectory.]]&lt;br /&gt;
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The reactive trajectory was found using initial conditions of r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.48 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.74 Å, while momenta were set to 0.&lt;br /&gt;
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As F approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and forms a bond with the atom, its potential energy increases, and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, the leaving atom, loses potential energy and gains kinetic energy.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Reactive_trajectory.png&amp;diff=615251</id>
		<title>File:Reactive trajectory.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Reactive_trajectory.png&amp;diff=615251"/>
		<updated>2017-05-05T14:40:26Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
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&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615176</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615176"/>
		<updated>2017-05-05T14:23:48Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
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&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
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This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
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== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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Trajectories with the following momenta combination were run while p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Reactivity&lt;br /&gt;
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| -1.25 || -2.5 || Reactive&lt;br /&gt;
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| -1.5  || -2.0 || Unreactive&lt;br /&gt;
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| -1.5  || -2.5 || Unreactive&lt;br /&gt;
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| -2.5  || -5.0 || Unreactive&lt;br /&gt;
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| -2.5  || -5.2 || Reactive&lt;br /&gt;
|}&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
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== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;br /&gt;
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=== &#039;&#039;&#039;Classifying endothermic and exothermic reactions&#039;&#039;&#039; ===&lt;br /&gt;
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In the H + HF reaction, the bond breaking is between the hydrogen and fluorine atoms. The H-F bond is relatively stronger due to a large difference of electronegativities between that of hyrodgen and fluorine atoms. Fluorine attracts the hydrogen atom stronger. Thus a large amount of energy is required to break the bond, and this makes the H + HF reaction endothermic.&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the bond breaking is between the two hydrogen atoms. The H-H bond is relatively weaker due to an approximately zero difference of electronegativities between the two atoms. A smaller amount of energy is required to break the H-H bond, thus the reaction is exothermic.&lt;br /&gt;
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=== &#039;&#039;&#039;The transition state&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Ts_estimation_distance-time.png|left|thumb|325x325px|The internuclear distance vs time plot at which the transition state occurs.]]&lt;br /&gt;
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The plot on the left illustrates the transition state of an F - H - H reaction, and it occurs when r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.811 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.744 Å, and the initial momenta set to 0.&lt;br /&gt;
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=== &#039;&#039;&#039;Activation energies&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:EA_hh_%2B_f.png|left|thumb|325x325px|The surface plot showing the saddle point in the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.]]&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the transition state resembles the reactants more due to its exothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the reactants is equal to the activation energy. The activation energy is found to be 22.574 kcal/mol.&lt;br /&gt;
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[[File:EA_hf_%2B_h.png|left|thumb|325x325px|The surface plot showing the saddle point in the H + HF reaction.]]&lt;br /&gt;
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In the H + HF reaction, the transition state resembles the products more due to its endothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the products is equal to the activation energy. The activation energy was found to be 28 kcal/mol.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615174</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615174"/>
		<updated>2017-05-05T14:23:01Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* Reactive and Unreactive Trajectories */&lt;/p&gt;
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&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
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This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
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== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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Trajectories with the following momenta combination were run while p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! Reactivity&lt;br /&gt;
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| -1.25 || -2.5 || Reactive&lt;br /&gt;
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| -1.5  || -2.0 || Unreactive&lt;br /&gt;
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| -1.5  || -2.5 || Unreactive&lt;br /&gt;
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| -2.5  || -5.0 || Unreactive&lt;br /&gt;
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| -2.5  || -5.2 || Reactive&lt;br /&gt;
|}&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
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== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;br /&gt;
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=== &#039;&#039;&#039;Classifying endothermic and exothermic reactions&#039;&#039;&#039; ===&lt;br /&gt;
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In the H + HF reaction, the bond breaking is between the hydrogen and fluorine atoms. The H-F bond is relatively stronger due to a large difference of electronegativities between that of hyrodgen and fluorine atoms. Fluorine attracts the hydrogen atom stronger. Thus a large amount of energy is required to break the bond, and this makes the H + HF reaction endothermic.&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the bond breaking is between the two hydrogen atoms. The H-H bond is relatively weaker due to an approximately zero difference of electronegativities between the two atoms. A smaller amount of energy is required to break the H-H bond, thus the reaction is exothermic.&lt;br /&gt;
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=== &#039;&#039;&#039;The transition state&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Ts_estimation_distance-time.png|left|thumb|325x325px|The internuclear distance vs time plot at which the transition state occurs.]]&lt;br /&gt;
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The plot on the left illustrates the transition state of an F - H - H reaction, and it occurs when r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.811 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.744 Å, and the initial momenta set to 0.&lt;br /&gt;
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=== &#039;&#039;&#039;Activation energies&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:EA_hh_%2B_f.png|left|thumb|325x325px|The surface plot showing the saddle point in the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.]]&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the transition state resembles the reactants more due to its exothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the reactants is equal to the activation energy. The activation energy is found to be 22.574 kcal/mol.&lt;br /&gt;
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[[File:EA_hf_%2B_h.png|left|thumb|325x325px|The surface plot showing the saddle point in the H + HF reaction.]]&lt;br /&gt;
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In the H + HF reaction, the transition state resembles the products more due to its endothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the products is equal to the activation energy. The activation energy was found to be 28 kcal/mol.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615127</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=615127"/>
		<updated>2017-05-05T14:11:23Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* F - H - H System */&lt;/p&gt;
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&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
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This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
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== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
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| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
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== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;br /&gt;
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=== &#039;&#039;&#039;Classifying endothermic and exothermic reactions&#039;&#039;&#039; ===&lt;br /&gt;
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In the H + HF reaction, the bond breaking is between the hydrogen and fluorine atoms. The H-F bond is relatively stronger due to a large difference of electronegativities between that of hyrodgen and fluorine atoms. Fluorine attracts the hydrogen atom stronger. Thus a large amount of energy is required to break the bond, and this makes the H + HF reaction endothermic.&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the bond breaking is between the two hydrogen atoms. The H-H bond is relatively weaker due to an approximately zero difference of electronegativities between the two atoms. A smaller amount of energy is required to break the H-H bond, thus the reaction is exothermic.&lt;br /&gt;
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=== &#039;&#039;&#039;The transition state&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Ts_estimation_distance-time.png|left|thumb|325x325px|The internuclear distance vs time plot at which the transition state occurs.]]&lt;br /&gt;
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The plot on the left illustrates the transition state of an F - H - H reaction, and it occurs when r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.811 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.744 Å, and the initial momenta set to 0.&lt;br /&gt;
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=== &#039;&#039;&#039;Activation energies&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:EA_hh_%2B_f.png|left|thumb|325x325px|The surface plot showing the saddle point in the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.]]&lt;br /&gt;
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In the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the transition state resembles the reactants more due to its exothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the reactants is equal to the activation energy. The activation energy is found to be 22.574 kcal/mol.&lt;br /&gt;
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[[File:EA_hf_%2B_h.png|left|thumb|325x325px|The surface plot showing the saddle point in the H + HF reaction.]]&lt;br /&gt;
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In the H + HF reaction, the transition state resembles the products more due to its endothermic nature. Thus the difference between the highest point of kinetic energy and the lowest point on the side of the products is equal to the activation energy. The activation energy was found to be 28 kcal/mol.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:EA_hh_%2B_f.png&amp;diff=615088</id>
		<title>File:EA hh + f.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:EA_hh_%2B_f.png&amp;diff=615088"/>
		<updated>2017-05-05T14:01:37Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
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&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:EA_hf_%2B_h.png&amp;diff=615045</id>
		<title>File:EA hf + h.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:EA_hf_%2B_h.png&amp;diff=615045"/>
		<updated>2017-05-05T13:51:52Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
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&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614886</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614886"/>
		<updated>2017-05-05T13:15:05Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* F - H - H System */&lt;/p&gt;
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&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
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This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
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== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
|}&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
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== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;br /&gt;
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=== &#039;&#039;&#039;Classifying endothermic and exothermic reactions&#039;&#039;&#039; ===&lt;br /&gt;
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In a H + HF reaction, the bond breaking is between the hydrogen and fluorine atoms. The H-F bond is relatively stronger due to a large difference of electronegativities between that of hyrodgen and fluorine atoms. Fluorine attracts the hydrogen atom stronger. Thus a large amount of energy is required to break the bond, and this makes the H + HF reaction endothermic.&lt;br /&gt;
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In a F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the bond breaking is between the two hydrogen atoms. The H-H bond is relatively weaker due to an approximately zero difference of electronegativities between the two atoms. A smaller amount of energy is required to break the H-H bond, thus the reaction is exothermic.&lt;br /&gt;
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=== &#039;&#039;&#039;The transition state&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:Ts_estimation_distance-time.png|left|thumb|325x325px|The internuclear distance vs time plot of an F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction at which the transition state occurs.]]&lt;br /&gt;
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The plot on the left illustrates the transition state of the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, and it occurs when r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt; = 1.811 Å and r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 0.744 Å, and the initial momenta set to 0.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Ts_estimation_distance-time.png&amp;diff=614868</id>
		<title>File:Ts estimation distance-time.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Ts_estimation_distance-time.png&amp;diff=614868"/>
		<updated>2017-05-05T13:08:09Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614849</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614849"/>
		<updated>2017-05-05T13:01:48Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
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This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
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== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
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== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;br /&gt;
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In a H + HF reaction, the bond breaking is between the hydrogen and fluorine atoms. The H-F bond is relatively stronger due to a large difference of electronegativities between that of hyrodgen and fluorine atoms. Fluorine attracts the hydrogen atom stronger. Thus a large amount of energy is required to break the bond, and this makes the H + HF reaction endothermic.&lt;br /&gt;
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In a F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, the bond breaking is between the two hydrogen atoms. The H-H bond is relatively weaker due to an approximately zero difference of electronegativities between the two atoms. A smaller amount of energy is required to break the H-H bond, thus the reaction is exothermic.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614809</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614809"/>
		<updated>2017-05-05T12:46:51Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
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&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
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This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
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== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614806</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614806"/>
		<updated>2017-05-05T12:45:23Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* F - H - H System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
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This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
|}&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
&lt;br /&gt;
This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
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== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614804</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614804"/>
		<updated>2017-05-05T12:44:58Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* H + H2 System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn.png|center]]&lt;br /&gt;
&lt;br /&gt;
The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
|}&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;br /&gt;
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== &#039;&#039;&#039;F - H - H System&#039;&#039;&#039; ==&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614801</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614801"/>
		<updated>2017-05-05T12:43:48Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* H + H2 System */&lt;/p&gt;
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&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
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This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
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== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
&lt;br /&gt;
The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
&lt;br /&gt;
The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
&lt;br /&gt;
This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
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[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway moves along the floor of the potential valley.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:4.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path that does not cross the saddle point - a path that makes the reaction feasible if the molecules have enough initial kinetic energy.&lt;br /&gt;
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H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; forms a bond with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; as the trajectory crosses past the saddle point but it moves back towards the initial path.&lt;br /&gt;
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The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond breaks again.&lt;br /&gt;
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[[File:5.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -2.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -5.2, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The trajectory moves along a different path and does not cross the saddle point.&lt;br /&gt;
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This path requires higher initial kinetic energy. The trajectory continues along the path down the floor of the other valley, after the formation of the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:5.png&amp;diff=614792</id>
		<title>File:5.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:5.png&amp;diff=614792"/>
		<updated>2017-05-05T12:40:13Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: Mhz15 uploaded a new version of File:5.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:4.png&amp;diff=614774</id>
		<title>File:4.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:4.png&amp;diff=614774"/>
		<updated>2017-05-05T12:33:46Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: Mhz15 uploaded a new version of File:4.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614769</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614769"/>
		<updated>2017-05-05T12:31:51Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* H + H2 System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
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This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
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== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
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[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
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The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
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The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
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The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
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At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
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[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
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The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
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The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
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[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
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The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
|}&lt;br /&gt;
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The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
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The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;br /&gt;
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=== &#039;&#039;&#039;Reactive and Unreactive Trajectories&#039;&#039;&#039; ===&lt;br /&gt;
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[[File:1.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.25, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway crosses the route along the floor of the potential valley, which is the path that requires the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H molecules to have relatively small initial kinetic energies.&lt;br /&gt;
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This pathway takes the reactant molecules to regions of least potential energy, as r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; increases as the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; atom approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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The trajectory continues its path as H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; moves away and the new H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms.&lt;br /&gt;
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[[File:2.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.0, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;br /&gt;
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The reaction pathway does not go along the floor of the potential valley - it stops at the point where the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule possesses equilibrium bond length.&lt;br /&gt;
&lt;br /&gt;
The H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond does not form.&lt;br /&gt;
&lt;br /&gt;
[[File:3.png|left|thumb|325x325px|Surface plot of the trajectory with conditions p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = -1.50, p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = -2.5, and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.]]&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:3.png&amp;diff=614766</id>
		<title>File:3.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:3.png&amp;diff=614766"/>
		<updated>2017-05-05T12:30:53Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: Mhz15 uploaded a new version of File:3.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:2.png&amp;diff=614759</id>
		<title>File:2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:2.png&amp;diff=614759"/>
		<updated>2017-05-05T12:27:46Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: Mhz15 uploaded a new version of File:2.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:1.png&amp;diff=614719</id>
		<title>File:1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:1.png&amp;diff=614719"/>
		<updated>2017-05-05T12:13:51Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: Mhz15 uploaded a new version of File:1.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614413</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=614413"/>
		<updated>2017-05-05T09:32:18Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* H + H2 System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn.png|center]]&lt;br /&gt;
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The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
&lt;br /&gt;
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=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
&lt;br /&gt;
The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
&lt;br /&gt;
The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
&lt;br /&gt;
The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
&lt;br /&gt;
The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
 &lt;br /&gt;
The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;br /&gt;
&lt;br /&gt;
The reaction path in mep refers to the trajectory along the minimum energy pathway.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=613420</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=613420"/>
		<updated>2017-05-04T13:51:04Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn.png|center]]&lt;br /&gt;
&lt;br /&gt;
The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
&lt;br /&gt;
The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
&lt;br /&gt;
The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
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The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
&lt;br /&gt;
The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
&lt;br /&gt;
The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
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The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
 &lt;br /&gt;
The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;br /&gt;
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=== &#039;&#039;&#039;Reaction Path&#039;&#039;&#039; ===&lt;br /&gt;
{|style=&amp;quot;margin: 0 auto;&amp;quot;&lt;br /&gt;
| [[File:Reaction_path_dynamics.png|thumb|325x325px|The reaction path in dynamics.]]&lt;br /&gt;
| [[File:Reaction-path-mep.png|thumb|325x325px|The reaction path in mep.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The above internuclear distance vs time plots show the path of the reaction starting from the transition state, when r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; = 0.9078 Å and r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; + 0.01 and the momenta p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; set to 0.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Reaction-path-mep.png&amp;diff=613308</id>
		<title>File:Reaction-path-mep.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Reaction-path-mep.png&amp;diff=613308"/>
		<updated>2017-05-04T13:06:07Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Reaction_path_dynamics.png&amp;diff=613293</id>
		<title>File:Reaction path dynamics.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Reaction_path_dynamics.png&amp;diff=613293"/>
		<updated>2017-05-04T12:58:22Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=613277</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=613277"/>
		<updated>2017-05-04T12:45:28Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* H + H2 System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn.png|center]]&lt;br /&gt;
&lt;br /&gt;
The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
&lt;br /&gt;
The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
&lt;br /&gt;
The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&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;
The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
&lt;br /&gt;
The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
&lt;br /&gt;
The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png|left|The internuclear distance vs time plot of the transition state.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
The plot on the left illustrates the trajectory of the transition state at r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; when r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is approximated to 0.9078 Å and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0.&lt;br /&gt;
 &lt;br /&gt;
The gradient of the trajectory is zero. The internuclear distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; is around 1.8 Å which agrees with the approximated value at which the transition state forms, as shown in the above still of the reaction animation.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png&amp;diff=613259</id>
		<title>File:1st rxn best-TS-estimate distance vs time USED.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:1st_rxn_best-TS-estimate_distance_vs_time_USED.png&amp;diff=613259"/>
		<updated>2017-05-04T12:32:51Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612756</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612756"/>
		<updated>2017-05-02T15:33:35Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* H + H2 System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn.png|center]]&lt;br /&gt;
&lt;br /&gt;
The reaction between an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule and an H atom is discussed below through the use of plots obtained from MATLAB.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
&lt;br /&gt;
The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
&lt;br /&gt;
The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&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;
=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&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;
The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
&lt;br /&gt;
The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
&lt;br /&gt;
The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:1st_rxn.png&amp;diff=612732</id>
		<title>File:1st rxn.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:1st_rxn.png&amp;diff=612732"/>
		<updated>2017-05-02T15:28:28Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612716</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612716"/>
		<updated>2017-05-02T15:22:17Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* Interpreting the Distance vs Time Plot */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
&lt;br /&gt;
The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
&lt;br /&gt;
The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&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;
=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&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;
The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;br /&gt;
&lt;br /&gt;
The H atoms in molecule H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (shown in red) maintain their oscillation while H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; moves closer towards H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, illustrated in blue.&lt;br /&gt;
&lt;br /&gt;
The potential energy of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;, relative to the two other H atoms, increases as it approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; up to a point - the transition state - where the the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; equals that of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
As has been mentioned above, H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; oscillates around H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, shown in blue, past the transition state, and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; gains kinetic energy as it moves away and loses potential energy.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612685</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612685"/>
		<updated>2017-05-02T15:09:40Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* H + H2 System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
&lt;br /&gt;
The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
&lt;br /&gt;
The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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=== &#039;&#039;&#039;Interpreting the Distance vs Time Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The animation still mentioned above ties in with the discussion of the H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction dynamics in terms of internuclear distance.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612656</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612656"/>
		<updated>2017-05-02T14:57:55Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* H + H2 System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond distance.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
&lt;br /&gt;
The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
&lt;br /&gt;
The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
=== &#039;&#039;&#039;Animation&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
=== &#039;&#039;&#039;Potential Energy vs Time&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_(ed)_distance_vs_time.png|left|The internuclear distance vs time plot.|thumb|325x325px]]&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:1st_rxn_(ed)_distance_vs_time.png&amp;diff=612647</id>
		<title>File:1st rxn (ed) distance vs time.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:1st_rxn_(ed)_distance_vs_time.png&amp;diff=612647"/>
		<updated>2017-05-02T14:53:39Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612638</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612638"/>
		<updated>2017-05-02T14:49:53Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* Animation */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs A-B bond distance.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
&lt;br /&gt;
The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
&lt;br /&gt;
The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&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;
=== &#039;&#039;&#039;Animation&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_transition_state_distance_-_LABELLED.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
At the beginning of the sequence, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;, decreases from ~2.3 Å to a minimum ~0.6 Å where it oscillates relative to the middle H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom.&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, corresponding to the internuclear distance of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;, increases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;. Eventually H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; breaks away from the attraction of H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; and moves away to a maximum r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The sequence shown on the left illustrates the transition state where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is equal to r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; at about 0.9 Å.&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:1st_rxn_transition_state_distance_-_LABELLED.png&amp;diff=612622</id>
		<title>File:1st rxn transition state distance - LABELLED.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:1st_rxn_transition_state_distance_-_LABELLED.png&amp;diff=612622"/>
		<updated>2017-05-02T14:43:18Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612596</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612596"/>
		<updated>2017-05-02T14:34:17Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* Animation */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs A-B bond distance.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
&lt;br /&gt;
The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
&lt;br /&gt;
The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&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;
=== &#039;&#039;&#039;Animation&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_transition_state_distance.png|left|A still from the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612589</id>
		<title>MRD:mhz15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:mhz15&amp;diff=612589"/>
		<updated>2017-05-02T14:33:10Z</updated>

		<summary type="html">&lt;p&gt;Mhz15: /* H + H2 System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== &#039;&#039;&#039;Introduction&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
This is the page created by Hafiz Zainal to report the results of his Molecular Reaction Dynamics simulation using MATLAB.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
=== &#039;&#039;&#039;Surface Plot&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_potential_energy_surface.png|left|A surface plot of potential energy vs A-B bond distance.|thumb|325x325px]]&lt;br /&gt;
&lt;br /&gt;
The surface plot on the left shows the variation of potential energy of an H atom in collision with an H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule.&lt;br /&gt;
&lt;br /&gt;
The blue-red spectrum corresponds to the potential energy range with blue being the minimum and red the maximum.&lt;br /&gt;
&lt;br /&gt;
The black wavy line illustrates the path of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; along the minimum vibrational energy of the diatomic molecule.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
=== &#039;&#039;&#039;Animation&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
[[File:1st_rxn_transition_state_distance.png|left|A still of the animated H - H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; collision sequence.|thumb|325x325px]]&lt;/div&gt;</summary>
		<author><name>Mhz15</name></author>
	</entry>
</feed>