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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811790</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811790"/>
		<updated>2020-05-22T22:42:54Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.9 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.9 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;br /&gt;
&lt;br /&gt;
=== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
Transition state thoery predictions will likely overestimate the predictions for rate, as it assumes all of the reaction goes to completion due to boltzmann distribution (all molecules have enough kinetic energy). Yet, it doesn&#039;t consider barrier recrossing, where the bond in the product forms, but they may reverse if they have a high enough vibrational energy. There is also the case that transition state theory treats energy classically, so ignores tunneling effects that could lower estimates. This effects is generally small, and is only really prevalent at low temperatures.&amp;lt;ref&amp;gt;Steinfeld, Jeffrey I, (1999) Chemical kinetics and dynamics, Prentice-Hall, p. 287-321&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H System ==&lt;br /&gt;
[[File:Surface Plot 01535442.png|thumb|312x312px|Figure 4: Contour plot of F-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system]]&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ===&lt;br /&gt;
==== F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
The reaction is exothermic, as the structure H-F is much more lower in energy, and there is noticable drop in the surface at the H-F product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The product formed, H-F, as bond energy of 565 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&amp;lt;ref name=&amp;quot;:0&amp;quot;&amp;gt;Huheey, pps. A-21 to A-34; T.L. Cottrell, &amp;quot;The Strengths of Chemical Bonds,&amp;quot; 2nd ed., Butterworths, London, 1958&amp;lt;/ref&amp;gt; This is higher than the bond energy of H-H, thus the products will be lower in energy than the reactants.  &lt;br /&gt;
&lt;br /&gt;
==== H + HF ====&lt;br /&gt;
This reaction is endothermic, as H-H is much higher in energy than H-F, and there surface of the potential curve is higher in the H-H product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The product formed, H-H, as a bond energy of 432 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&amp;lt;ref name=&amp;quot;:0&amp;quot; /&amp;gt; This is lower than the bond energy of H-F, thus the products should be higher in energy than the reactants. &lt;br /&gt;
[[File:Contour plot with Transtion State of F-H-H 0153442.png|thumb|Figure 5: Contour plot with approximate transtion state position for F-H-H system|300x300px]]&lt;br /&gt;
&lt;br /&gt;
=== Locate the approximate position of the transition state ===&lt;br /&gt;
The transition state positions is approximately at distance H - H = 74 pm and F - H = 181.4 pm. Initially, Hammond&#039;s Postulate was recalled, which states that the transition state of a reaction resembles the species more higher in energy, in this case either the product or the reactant. As we are observing the F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;system, it is exothermic and and will resemble H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants. The bond length of H-H is reported to be 74 pm, so this was kept the same, as well as keeping the momentums at 0, to find the position (see &#039;&#039;&#039;Figure 6 &#039;&#039;&#039;for depiction).&lt;br /&gt;
&lt;br /&gt;
=== Report the activation energy for both reactions ===&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system is 1.032 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and the for the H + HF system, the activation energy is -126.684 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. These were found by finding the difference between the potential energy of the transition state and the reactant, using both systems (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF) so the mep could be pathed (only to reactants). &lt;br /&gt;
&lt;br /&gt;
=== Reaction Dynamics ===&lt;br /&gt;
[[File:Momenta vs time 01535442.png|thumb|Figure 6: Momenta vs time graph of Reactive Trajectory|318x318px]]&lt;br /&gt;
&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy and explain how this could be confirmed experimentally ====&lt;br /&gt;
The reactive trajectory in this example is set by F - H = 230 pm, and H - H = 74 pm, with respective momentums being -13 and 0. In &#039;&#039;&#039;Figure 6&#039;&#039;&#039;, the momentum vs time graph of this system is displayed, where A-B = F - H, and B-C = H - H.  Initially, F - H has translational energy which enables it to move, and H - H has vibrational energy and is oscillating. Then, once the collision occurs, the momentums become postive, as the newly formed products move away. Now, F - H bond has vibrational energy, and it oscillatory behaviour is large, and the H - H momentum steadies as H moves away with translational energy. This can be confirmed by analysis of chemiluminescence and possibly IR.  &lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
The distributions of energy is influenced by the strength of both translational modes and vibrational modes. The biggest component to the favourability of the modes is the position of the transition state in the potential energy surface. If a reaction has a late transition state (occurs in product channel), then high translational energy trajectories will lead to succussful reactions. Yet, if a reaction has an early transition state (occurs in reactant channel), will favour vibration excitation of the molecule leading to a reactive trajectory.&amp;lt;ref&amp;gt;Steinfeld, Jeffrey I, (1999) Chemical kinetics and dynamics, Prentice-Hall, p. 272-274&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Biliography ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811777</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811777"/>
		<updated>2020-05-22T22:39:09Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy and explain how this could be confirmed experimentally */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.9 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.9 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;br /&gt;
&lt;br /&gt;
=== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
Transition state thoery predictions will likely overestimate the predictions for rate, as it assumes all of the reaction goes to completion due to boltzmann distribution (all molecules have enough kinetic energy). Yet, it doesn&#039;t consider barrier recrossing, where the bond in the product forms, but they may reverse if they have a high enough vibrational energy. There is also the case that transition state theory treats energy classically, so ignores tunneling effects that could lower estimates. This effects is generally small, and is only really prevalent at low temperatures.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H System ==&lt;br /&gt;
[[File:Surface Plot 01535442.png|thumb|312x312px|Figure 4: Contour plot of F-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system]]&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ===&lt;br /&gt;
==== F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
The reaction is exothermic, as the structure H-F is much more lower in energy, and there is noticable drop in the surface at the H-F product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The product formed, H-F, as bond energy of 565 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&amp;lt;ref name=&amp;quot;:0&amp;quot;&amp;gt;Huheey, pps. A-21 to A-34; T.L. Cottrell, &amp;quot;The Strengths of Chemical Bonds,&amp;quot; 2nd ed., Butterworths, London, 1958&amp;lt;/ref&amp;gt; This is higher than the bond energy of H-H, thus the products will be lower in energy than the reactants.  &lt;br /&gt;
&lt;br /&gt;
==== H + HF ====&lt;br /&gt;
This reaction is endothermic, as H-H is much higher in energy than H-F, and there surface of the potential curve is higher in the H-H product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The product formed, H-H, as a bond energy of 432 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&amp;lt;ref name=&amp;quot;:0&amp;quot; /&amp;gt; This is lower than the bond energy of H-F, thus the products should be higher in energy than the reactants. &lt;br /&gt;
[[File:Contour plot with Transtion State of F-H-H 0153442.png|thumb|Figure 5: Contour plot with approximate transtion state position for F-H-H system|300x300px]]&lt;br /&gt;
&lt;br /&gt;
=== Locate the approximate position of the transition state ===&lt;br /&gt;
The transition state positions is approximately at distance H - H = 74 pm and F - H = 181.4 pm. Initially, Hammond&#039;s Postulate was recalled, which states that the transition state of a reaction resembles the species more higher in energy, in this case either the product or the reactant. As we are observing the F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;system, it is exothermic and and will resemble H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants. The bond length of H-H is reported to be 74 pm, so this was kept the same, as well as keeping the momentums at 0, to find the position (see &#039;&#039;&#039;Figure 6 &#039;&#039;&#039;for depiction).&lt;br /&gt;
&lt;br /&gt;
=== Report the activation energy for both reactions ===&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system is 1.032 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and the for the H + HF system, the activation energy is -126.684 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. These were found by finding the difference between the potential energy of the transition state and the reactant, using both systems (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF) so the mep could be pathed (only to reactants). &lt;br /&gt;
&lt;br /&gt;
=== Reaction Dynamics ===&lt;br /&gt;
[[File:Momenta vs time 01535442.png|thumb|Figure 6: Momenta vs time graph of Reactive Trajectory|318x318px]]&lt;br /&gt;
&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy and explain how this could be confirmed experimentally ====&lt;br /&gt;
The reactive trajectory in this example is set by F - H = 230 pm, and H - H = 74 pm, with respective momentums being -13 and 0. In &#039;&#039;&#039;Figure 6&#039;&#039;&#039;, the momentum vs time graph of this system is displayed, where A-B = F - H, and B-C = H - H.  Initially, F - H has translational energy which enables it to move, and H - H has vibrational energy and is oscillating. Then, once the collision occurs, the momentums become postive, as the newly formed products move away. Now, F - H bond has vibrational energy, and it oscillatory behaviour is large, and the H - H momentum steadies as H moves away with translational energy. This can be confirmed by analysis of chemiluminescence and possibly IR.  &lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
The distributions of energy is influenced by the strength of both translational modes and vibrational modes. The biggest component to the favourability of the modes is the position of the transition state in the potential energy surface. If a reaction has a late transition state (occurs in product channel), then high translational energy trajectories will lead to succussful reactions. Yet, if a reaction has an early transition state (occurs in reactant channel), will favour vibration excitation of the molecule leading to a reactive trajectory.&amp;lt;ref&amp;gt;Steinfeld, Jeffrey I, (1999) Chemical kinetics and dynamics, Prentice-Hall, p. 272-274&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Biliography ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811653</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811653"/>
		<updated>2020-05-22T21:50:02Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy and explain how this could be confirmed experimentally */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.9 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.9 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;br /&gt;
&lt;br /&gt;
=== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H System ==&lt;br /&gt;
[[File:Surface Plot 01535442.png|thumb|312x312px|Figure 4: Contour plot of F-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system]]&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ===&lt;br /&gt;
==== F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
The reaction is exothermic, as the structure H-F is much more lower in energy, and there is noticable drop in the surface at the H-F product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The product formed, H-F, as bond energy of 565 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is higher than the bond energy of H-H, thus the products will be lower in energy than the reactants.  &lt;br /&gt;
&lt;br /&gt;
==== H + HF ====&lt;br /&gt;
This reaction is endothermic, as H-H is much higher in energy than H-F, and there surface of the potential curve is higher in the H-H product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The product formed, H-H, as a bond energy of 432 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is lower than the bond energy of H-F, thus the products should be higher in energy than the reactants. &lt;br /&gt;
[[File:Contour plot with Transtion State of F-H-H 0153442.png|thumb|Figure 5: Contour plot with approximate transtion state position for F-H-H system|300x300px]]&lt;br /&gt;
&lt;br /&gt;
=== Locate the approximate position of the transition state ===&lt;br /&gt;
The transition state positions is approximately at distance H - H = 74 pm and F - H = 181.4 pm. Initially, Hammond&#039;s Postulate was recalled, which states that the transition state of a reaction resembles the species more higher in energy, in this case either the product or the reactant. As we are observing the F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;system, it is exothermic and and will resemble H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants. The bond length of H-H is reported to be 74 pm, so this was kept the same, as well as keeping the momentums at 0, to find the position (see &#039;&#039;&#039;Figure 6 &#039;&#039;&#039;for depiction).&lt;br /&gt;
&lt;br /&gt;
=== Report the activation energy for both reactions ===&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system is 1.032 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and the for the H + HF system, the activation energy is -126.684 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. These were found by finding the difference between the potential energy of the transition state and the reactant, using both systems (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF) so the mep could be pathed (only to reactants). &lt;br /&gt;
&lt;br /&gt;
=== Reaction Dynamics ===&lt;br /&gt;
[[File:Momenta vs time 01535442.png|thumb|Figure 6: Momenta vs time graph of Reactive Trajectory]]&lt;br /&gt;
&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy and explain how this could be confirmed experimentally ====&lt;br /&gt;
The reactive trajectory in this example is set by F - H = 230 pm, and H - H = 74 pm, with respective momentums being -13 and 0.  &lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
The distributions of energy is influenced by the strength of both translational modes and vibrational modes. The biggest component to the favourability of the modes in the position of the transition state in potential energy surface. If a reaction has a late transition state (occurs in product channel), then high translational energy trajectories will lead to succussful reactions. This is seen by the&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Momenta_vs_time_01535442.png&amp;diff=811647</id>
		<title>File:Momenta vs time 01535442.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Momenta_vs_time_01535442.png&amp;diff=811647"/>
		<updated>2020-05-22T21:48:19Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811631</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811631"/>
		<updated>2020-05-22T21:44:23Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.9 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.9 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;br /&gt;
&lt;br /&gt;
=== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H System ==&lt;br /&gt;
[[File:Surface Plot 01535442.png|thumb|260x260px|Figure 4: Contour plot of F-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system]]&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ===&lt;br /&gt;
==== F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
The reaction is exothermic, as the structure H-F is much more lower in energy, and there is noticable drop in the surface at the H-F product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The product formed, H-F, as bond energy of 565 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is higher than the bond energy of H-H, thus the products will be lower in energy than the reactants.  &lt;br /&gt;
&lt;br /&gt;
==== H + HF ====&lt;br /&gt;
This reaction is endothermic, as H-H is much higher in energy than H-F, and there surface of the potential curve is higher in the H-H product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The product formed, H-H, as a bond energy of 432 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is lower than the bond energy of H-F, thus the products should be higher in energy than the reactants. &lt;br /&gt;
[[File:Contour plot with Transtion State of F-H-H 0153442.png|thumb|Figure 6: Contour plot with approximate transtion state position for F-H-H system|249x249px]]&lt;br /&gt;
&lt;br /&gt;
=== Locate the approximate position of the transition state ===&lt;br /&gt;
The transition state positions is approximately at distance H - H = 74 pm and F - H = 181.4 pm. Initially, Hammond&#039;s Postulate was recalled, which states that the transition state of a reaction resembles the species more higher in energy, in this case either the product or the reactant. As we are observing the F + H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;system, it is exothermic and and will resemble H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants. The bond length of H-H is reported to be 74 pm, so this was kept the same, as well as keeping the momentums at 0, to find the position (see &#039;&#039;&#039;Figure 6 &#039;&#039;&#039;for depiction).&lt;br /&gt;
&lt;br /&gt;
=== Report the activation energy for both reactions ===&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system is 1.032 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and the for the H + HF system, the activation energy is -126.684 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. These were found by finding the difference between the potential energy of the transition state and the reactant, using both systems (F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF) so the mep could be pathed (only to reactants). &lt;br /&gt;
&lt;br /&gt;
=== Reaction Dynamics ===&lt;br /&gt;
&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy and explain how this could be confirmed experimentally ====&lt;br /&gt;
The reactive trajectory in this example is set by F - H = 230 pm, and H - H = 74 pm, with respective momentums being -13 and 0. &lt;br /&gt;
&lt;br /&gt;
==== Explain how this could be confirmed experimentally ====&lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
The distributions of energy is influenced by the strength of both translational modes and vibrational modes. The biggest component to the favourability of the modes in the position of the transition state in potential energy surface. If a reaction has a late transition state (occurs in product channel), then high translational energy trajectories will lead to succussful reactions. This is seen by the&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811222</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811222"/>
		<updated>2020-05-22T19:41:21Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.9 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.9 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;br /&gt;
&lt;br /&gt;
=== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H System ==&lt;br /&gt;
[[File:Surface Plot 01535442.png|thumb|270x270px|Figure 4: Contour plot of F-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system]]&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ===&lt;br /&gt;
==== F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
The reaction is exothermic, as the structure H-F is much more lower in energy, and there is noticable drop in the surface at the H-F product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The product formed, H-F, as bond energy of 565 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is higher than the bond energy of H-H, thus the products will be lower in energy than the reactants.  &lt;br /&gt;
&lt;br /&gt;
==== H + HF ====&lt;br /&gt;
This reaction is endothermic, as H-H is much higher in energy than H-F, and there surface of the potential curve is higher in the H-H product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The product formed, H-H, as a bond energy of 432 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. This is lower than the bond energy of H-F, thus the products should be higher in energy than the reactants. &lt;br /&gt;
[[File:Contour plot with Transtion State of F-H-H 0153442.png|thumb|Figure 6: Contour plot with approximate transtion state position for F-H-H system|257x257px]]&lt;br /&gt;
&lt;br /&gt;
=== Locate the approximate position of the transition state ===&lt;br /&gt;
The transition state positions is approximately at distance H - H = 73 pm and F - H = 182 pm (see &#039;&#039;&#039;Figure 6 &#039;&#039;&#039;for depiction).&lt;br /&gt;
&lt;br /&gt;
=== Report the activation energy for both reactions ===&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system is 1.032 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and the for the H + HF system, the activation energy is 126.684 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
=== Reaction Dynamics ===&lt;br /&gt;
&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy ====&lt;br /&gt;
Placeholder&lt;br /&gt;
&lt;br /&gt;
==== Explain how this could be confirmed experimentally ====&lt;br /&gt;
Placefolder&lt;br /&gt;
&lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
The distributions of energy is influenced by the strength of both translational modes and vibrational modes. The biggest component to the favourability of the modes in the position of the transition state in potential energy surface.&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811184</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811184"/>
		<updated>2020-05-22T19:33:06Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Report the activation energy for both reactions */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.9 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.9 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;br /&gt;
&lt;br /&gt;
=== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H System ==&lt;br /&gt;
[[File:Surface Plot 01535442.png|thumb|270x270px|Figure 4: Contour plot of F-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system]]&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ===&lt;br /&gt;
==== F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
The reaction is exothermic, as the structure H-F is much more lower in energy, and there is noticable drop in the surface at the H-F product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The reaction is also a lot lower in total energy than forming H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;from H-F (-345.593 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;). &lt;br /&gt;
&lt;br /&gt;
==== H + HF ====&lt;br /&gt;
This reaction is endothermic, as H-H is much higher in energy than H-F, and there surface of the potential curve is higher in the H-H product channel (&#039;&#039;&#039;Figure 5&#039;&#039;&#039;). The reactions is a lot higher in total energy (199.091 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;).&lt;br /&gt;
[[File:Contour plot with Transtion State of F-H-H 0153442.png|thumb|Figure 6: Contour plot with approximate transtion state position for F-H-H system|257x257px]]&lt;br /&gt;
&lt;br /&gt;
=== Locate the approximate position of the transition state ===&lt;br /&gt;
The transition state positions is approximately at distance H - H = 73 pm and F - H = 182 pm (see &#039;&#039;&#039;Figure 6 &#039;&#039;&#039;for depiction).&lt;br /&gt;
&lt;br /&gt;
=== Report the activation energy for both reactions ===&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system is 1.032 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and the for the H + HF system, the activation energy is 126.684 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
=== Reaction Dynamics ===&lt;br /&gt;
&lt;br /&gt;
==== In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy ====&lt;br /&gt;
Placeholder&lt;br /&gt;
&lt;br /&gt;
==== Explain how this could be confirmed experimentally ====&lt;br /&gt;
Placefolder&lt;br /&gt;
&lt;br /&gt;
==== Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state ====&lt;br /&gt;
The distributions of energy is influenced by the strength of both translational modes and vibrational modes. The biggest component to the favourability of the modes in the position of the transition state in potential energy surface.&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Surface_Plot_01535442.png&amp;diff=811180</id>
		<title>File:Surface Plot 01535442.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Surface_Plot_01535442.png&amp;diff=811180"/>
		<updated>2020-05-22T19:32:39Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811075</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=811075"/>
		<updated>2020-05-22T18:56:54Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Report the activation energy for both reactions */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.9 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.9 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;br /&gt;
&lt;br /&gt;
=== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H System ==&lt;br /&gt;
[[File:Contour Plot of F-H2 01535442.png|thumb|259x259px|Figure 4: Contour plot of F-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system|left]]&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ===&lt;br /&gt;
[[File:Contour Plot of H-HF 01535442.png|thumb|269x269px|Figure 5: Contour plot of F-HF system]]&lt;br /&gt;
==== F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
The reaction is exothermic, as the structure H-F is much more lower in energy, and there is noticable drop in the surface at the H-F product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The reaction is also a lot lower in total energy than forming H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;from H-F (-345.593 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;). &lt;br /&gt;
&lt;br /&gt;
==== H + HF ====&lt;br /&gt;
This reaction is endothermic, as H-H is much higher in energy than H-F, and there surface of the potential curve is higher in the H-H product channel (&#039;&#039;&#039;Figure 5&#039;&#039;&#039;). The reactions is a lot higher in total energy (199.091 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;).&lt;br /&gt;
[[File:Contour plot with Transtion State of F-H-H 0153442.png|left|thumb|Figure 6: Contour plot with approximate transtion state position for F-H-H system|257x257px]]&lt;br /&gt;
&lt;br /&gt;
=== Locate the approximate position of the transition state ===&lt;br /&gt;
The transition state positions is approximately at distance H - H = 73 pm and F - H = 182 pm (see &#039;&#039;&#039;Figure 6 &#039;&#039;&#039;for depiction).&lt;br /&gt;
&lt;br /&gt;
=== Report the activation energy for both reactions ===&lt;br /&gt;
The activation energy for the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system is 1.032 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, and the for the H + HF system, the activation energy is 126.684 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=810770</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=810770"/>
		<updated>2020-05-22T17:40:35Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Locate the approximate position of the transition state */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.9 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.9 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;br /&gt;
&lt;br /&gt;
=== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H System ==&lt;br /&gt;
[[File:Contour Plot of F-H2 01535442.png|thumb|259x259px|Figure 4: Contour plot of F-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system|left]]&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ===&lt;br /&gt;
[[File:Contour Plot of H-HF 01535442.png|thumb|269x269px|Figure 5: Contour plot of F-HF system]]&lt;br /&gt;
==== F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
The reaction is exothermic, as the structure H-F is much more lower in energy, and there is noticable drop in the surface at the H-F product channel (&#039;&#039;&#039;Figure 4&#039;&#039;&#039;). The reaction is also a lot lower in total energy than forming H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;from H-F (-345.593 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;). &lt;br /&gt;
&lt;br /&gt;
==== H + HF ====&lt;br /&gt;
This reaction is endothermic, as H-H is much higher in energy than H-F, and there surface of the potential curve is higher in the H-H product channel (&#039;&#039;&#039;Figure 5&#039;&#039;&#039;). The reactions is a lot higher in total energy (199.091 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;).&lt;br /&gt;
[[File:Contour plot with Transtion State of F-H-H 0153442.png|left|thumb|Figure 6: Contour plot with approximate transtion state position for F-H-H system|257x257px]]&lt;br /&gt;
&lt;br /&gt;
=== Locate the approximate position of the transition state ===&lt;br /&gt;
The transition state positions is approximately at distance H - H = 73 pm and F - H = 182 pm (see &#039;&#039;&#039;Figure 6 &#039;&#039;&#039;for depiction).&lt;br /&gt;
&lt;br /&gt;
=== Report the activation energy for both reactions ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=810705</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=810705"/>
		<updated>2020-05-22T17:23:25Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Locate the approximate position of the transition state */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;br /&gt;
&lt;br /&gt;
=== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H System ==&lt;br /&gt;
[[File:Contour Plot of F-H2 01535442.png|thumb|289x289px|Figure 4: Contour plot of F-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system]]&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ===&lt;br /&gt;
&lt;br /&gt;
==== F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
The reaction is exothermic, as the structure H-F is much more lower in energy, and there is noticable drop in the surface at the H-F product channel. The reaction is also a lot lower in total energy than forming H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;from H-F (-345.593 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;). &lt;br /&gt;
&lt;br /&gt;
==== H + HF ====&lt;br /&gt;
This reaction is endothermic, as H-H is much higher in energy than H-F, and there surface of the potential curve is higher in the H-H product channel. The reactions is a lot higher in total energy (199.091 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;).&lt;br /&gt;
[[File:Contour plot with Transtion State of F-H-H 0153442.png|left|thumb|Figure 6: Contour plot with approximate transtion state position for F-H-H system]]&lt;br /&gt;
&lt;br /&gt;
=== Locate the approximate position of the transition state ===&lt;br /&gt;
[[File:Contour Plot of H-HF 01535442.png|thumb|290x290px|Figure 5: Contour plot of F-HF system]]&lt;br /&gt;
The transition state positions is approximately at distance H - H = 73 pm and F - H = 182 pm.&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_plot_with_Transtion_State_of_F-H-H_0153442.png&amp;diff=810698</id>
		<title>File:Contour plot with Transtion State of F-H-H 0153442.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_plot_with_Transtion_State_of_F-H-H_0153442.png&amp;diff=810698"/>
		<updated>2020-05-22T17:21:40Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=810680</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=810680"/>
		<updated>2020-05-22T17:19:05Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* F + H2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;br /&gt;
&lt;br /&gt;
=== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H System ==&lt;br /&gt;
[[File:Contour Plot of F-H2 01535442.png|thumb|289x289px|Figure 4: Contour plot of F-H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system]]&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ===&lt;br /&gt;
&lt;br /&gt;
==== F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
The reaction is exothermic, as the structure H-F is much more lower in energy, and there is noticable drop in the surface at the H-F product channel. The reaction is also a lot lower in total energy than forming H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;from H-F (-345.593 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;). &lt;br /&gt;
&lt;br /&gt;
==== H + HF ====&lt;br /&gt;
This reaction is endothermic, as H-H is much higher in energy than H-F, and there surface of the potential curve is higher in the H-H product channel. The reactions is a lot higher in total energy (199.091 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
=== Locate the approximate position of the transition state ===&lt;br /&gt;
[[File:Contour Plot of H-HF 01535442.png|thumb|290x290px|Figure 5: Contour plot of F-HF system]]&lt;br /&gt;
The transition state positions is approximately at distance H - H = 73 pm and F - H = 182 pm.&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_H-HF_01535442.png&amp;diff=810677</id>
		<title>File:Contour Plot of H-HF 01535442.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_H-HF_01535442.png&amp;diff=810677"/>
		<updated>2020-05-22T17:18:23Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: &lt;/p&gt;
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		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_F-H2_01535442.png&amp;diff=810667</id>
		<title>File:Contour Plot of F-H2 01535442.png</title>
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		<updated>2020-05-22T17:16:45Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: Tr1318 uploaded a new version of File:Contour Plot of F-H2 01535442.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_F-H2_01535442.png&amp;diff=810663</id>
		<title>File:Contour Plot of F-H2 01535442.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_F-H2_01535442.png&amp;diff=810663"/>
		<updated>2020-05-22T17:16:03Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: &lt;/p&gt;
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		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=810655</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=810655"/>
		<updated>2020-05-22T17:14:14Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Locate the approximate position of the transition state */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;br /&gt;
&lt;br /&gt;
=== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H System ==&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ===&lt;br /&gt;
&lt;br /&gt;
==== F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
The reaction is exothermic, as the structure H-F is much more lower in energy, and there is noticable drop in the surface at the H-F product channel. The reaction is also a lot lower in total energy than forming H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;from H-F (-345.593 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;). &lt;br /&gt;
&lt;br /&gt;
==== H + HF ====&lt;br /&gt;
This reaction is endothermic, as H-H is much higher in energy than H-F, and there surface of the potential curve is higher in the H-H product channel. The reactions is a lot higher in total energy (199.091 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
=== Locate the approximate position of the transition state ===&lt;br /&gt;
The transition state positions is approximately at distance H - H = 73 pm and F - H = 182 pm.&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809975</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809975"/>
		<updated>2020-05-22T12:39:13Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* What can you conclude from the table? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;br /&gt;
&lt;br /&gt;
=== Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values? ===&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H System ==&lt;br /&gt;
&lt;br /&gt;
=== By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved? ===&lt;br /&gt;
&lt;br /&gt;
==== F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ====&lt;br /&gt;
The reaction is exothermic, as the structure H-F is much more lower in energy, and there is noticable drop in the surface at the H-F product channel. The reaction is also a lot lower in total energy than forming H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;from H-F (-345.593 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;). &lt;br /&gt;
&lt;br /&gt;
==== H + HF ====&lt;br /&gt;
This reaction is endothermic, as H-H is much higher in energy than H-F, and there surface of the potential curve is higher in the H-H product channel. The reactions is a lot higher in total energy (199.091 kJ mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
=== Locate the approximate position of the transition state ===&lt;br /&gt;
The transition state is approximately&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809648</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809648"/>
		<updated>2020-05-22T10:24:15Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* On a potential energy surface diagram, how is the transition state mathematically defined? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|246x246px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|244x244px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809645</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809645"/>
		<updated>2020-05-22T10:23:32Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Comment on how the mep and the trajectory you just calculated differ */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|254x254px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|245x245px]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809643</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809643"/>
		<updated>2020-05-22T10:21:37Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* What can you conclude from the table? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|254x254px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px|left]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left|245x245px]]&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and so there is little oscillatory behaviour. When it gets to the transition state, there is reintroduction of oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively similiar levels of momentum to H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;. H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; has more visible oscillations in it&#039;s trajectory. The path does not reach the transition state, as there is not enough kinetic energy for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to form a bond with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, and repulsion forces between them push them apart, oscillating back to the reactant snapshot.&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is some oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond.There is then increased oscillatory behaviour in H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;, due to excess vibrational energy.&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, as it overcomes the repulsion to form a new bond. Yet, as momentum is high, there is large oscillations in the path 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;, so much so that new bond then breaks and reforms the reactants, oscillating backwards.&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;) molecule has relatively lower momentum than H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;, and there is little oscillatory behaviour with H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt;. There is enough momentum for H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; to reach the transition state, and there is few larger oscillations where the new bond between H&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is formed, and then this breaks and the reactant H&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;c&amp;lt;/sub&amp;gt; reforms. The reactant bond than breaks and reforms 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; molecule, and the path goes towards the products.&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;br /&gt;
In summary, the main influence on whether a trajectory will lead to a reaction is that the momentum p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; must be larger than p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, and around double the magnitude of p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;. The higher that values of momentum, the higher the kinetic energy in the system and the higher the total energy becomes.&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809583</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809583"/>
		<updated>2020-05-22T09:47:46Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|254x254px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px|left]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left|245x245px]]&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809570</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809570"/>
		<updated>2020-05-22T09:37:29Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|254x254px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px|left]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left|245x245px]]&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-357.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of Row 4 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of Row 5 01535442.png|frameless]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_Row_5_01535442.png&amp;diff=809568</id>
		<title>File:Contour Plot of Row 5 01535442.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_Row_5_01535442.png&amp;diff=809568"/>
		<updated>2020-05-22T09:37:01Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_Row_4_01535442.png&amp;diff=809559</id>
		<title>File:Contour Plot of Row 4 01535442.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_Row_4_01535442.png&amp;diff=809559"/>
		<updated>2020-05-22T09:32:31Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809555</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809555"/>
		<updated>2020-05-22T09:29:46Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|254x254px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px|left]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left|245x245px]]&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of Row 3 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_Row_3_01535442.png&amp;diff=809245</id>
		<title>File:Contour Plot of Row 3 01535442.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_Row_3_01535442.png&amp;diff=809245"/>
		<updated>2020-05-22T01:03:49Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809244</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809244"/>
		<updated>2020-05-22T01:02:25Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|254x254px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px|left]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left|245x245px]]&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.280&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|No&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of Row 2 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_Row_2_01535442.png&amp;diff=809243</id>
		<title>File:Contour Plot of Row 2 01535442.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_Row_2_01535442.png&amp;diff=809243"/>
		<updated>2020-05-22T01:01:11Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809242</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809242"/>
		<updated>2020-05-22T00:58:14Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Comment on how the mep and the trajectory you just calculated differ */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|254x254px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px|left]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left|245x245px]]&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.28&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809241</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809241"/>
		<updated>2020-05-22T00:57:34Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Exercise 1: H + H2 System */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|254x254px]]&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px|left]]&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left|245x245px]]&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.28&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809240</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809240"/>
		<updated>2020-05-22T00:56:21Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Comment on how the mep and the trajectory you just calculated differ */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|302x302px]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|245x245px|left]]&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left|245x245px]]&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.28&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809239</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809239"/>
		<updated>2020-05-22T00:52:35Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Comment on how the mep and the trajectory you just calculated differ */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|&#039;&#039;&#039;Figure 2&#039;&#039;&#039;: Contour plot of system displaced from transtition state. Calculation type: Dynamics|318x318px]]&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left]][[File:Internuclear Dist vs Time for rts 1535442.png|thumb|&amp;lt;b&amp;gt;Figure 1&amp;lt;/b&amp;gt;: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|centre|302x302px]]&lt;br /&gt;
&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.28&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809238</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809238"/>
		<updated>2020-05-22T00:50:51Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|Figure 2: Contour plot of system displaced from transtition state. Calculation type: Dynamics]]&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|&#039;&#039;&#039;Figure 3&#039;&#039;&#039;: Contour plot of system displaced from transtion state. Calculation type: MEP|left]][[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;|centre]]&lt;br /&gt;
&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.28&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809237</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809237"/>
		<updated>2020-05-22T00:49:20Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|thumb|Figure 2: Contour plot of system displaced from transtition state. Calculation type: Dynamics]]&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|&#039;&#039;&#039;Figure 3&#039;&#039;&#039;: Contour plot of system displaced from transtion state. Calculation type: MEP|left]]&lt;br /&gt;
&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.28&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809236</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809236"/>
		<updated>2020-05-22T00:46:26Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Figure 2: Contour plot of system displaced from transtition state. Calculation type: Dynamics]]&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left]]&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.28&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809235</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809235"/>
		<updated>2020-05-22T00:44:20Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Comment on how the mep and the trajectory you just calculated differ */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. [[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Figure 2: Contour plot of system displaced from transtition state. Calculation type: Dynamics]]&lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left]]&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.28&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809234</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809234"/>
		<updated>2020-05-22T00:43:14Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Figure 2: Contour plot of system displaced from transtition state. Calculation type: Dynamics]]&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left]]&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-414.28&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Yes&lt;br /&gt;
|&lt;br /&gt;
|[[File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png|frameless]]&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_P1%3D-2.56_P2%3D-5.1_01535442.png&amp;diff=809232</id>
		<title>File:Contour Plot of P1=-2.56 P2=-5.1 01535442.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_P1%3D-2.56_P2%3D-5.1_01535442.png&amp;diff=809232"/>
		<updated>2020-05-22T00:39:43Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809224</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809224"/>
		<updated>2020-05-22T00:16:30Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Figure 2: Contour plot of system displaced from transtition state. Calculation type: Dynamics]]&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left]]&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
&lt;br /&gt;
=== Complete the table below by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/ g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
!E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;&lt;br /&gt;
!Reactive?&lt;br /&gt;
!Description of the dynamics&lt;br /&gt;
!Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-2.56&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-4.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-3.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-5.1&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&amp;lt;nowiki&amp;gt;-10.6&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809219</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809219"/>
		<updated>2020-05-22T00:12:43Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Figure 2: Contour plot of system displaced from transtition state. Calculation type: Dynamics]]&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left]]&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
&lt;br /&gt;
=== Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
| -2.56 || -5.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || || || ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || || || ||&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809217</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809217"/>
		<updated>2020-05-22T00:12:22Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Comment on how the mep and the trajectory you just calculated differ */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Figure 2: Contour plot of system displaced from transtition state. Calculation type: Dynamics]]&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left]]&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;br /&gt;
&lt;br /&gt;
=== Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!&lt;br /&gt;
!&lt;br /&gt;
!&lt;br /&gt;
!&lt;br /&gt;
!&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== What can you conclude from the table? ===&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809213</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809213"/>
		<updated>2020-05-22T00:09:50Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Comment on how the mep and the trajectory you just calculated differ */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Figure 2: Contour plot of system displaced from transtition state. Calculation type: Dynamics]]&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left]]&lt;br /&gt;
The minimum energy path or mep takes a path through the potential surface where it does not move up or down the contour, rather it takes the the path of lowest energy througout (see &#039;&#039;&#039;Figure 2&#039;&#039;&#039;). The trajectory calculated by dynamics (&#039;&#039;&#039;Figure 3&#039;&#039;&#039;) follows the same overall path as the mep, though it&#039;s much more wavy. This is due to the vibration of the diatomic molecule. Conservation of energy is present in both as the dynamic trajectory oscillates between the same energy contours.&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809201</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809201"/>
		<updated>2020-05-21T23:27:06Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, showing estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. It can be distinguished from a local minimum by looking at the second derivative, which will be positive when the function is a local minimum, and negative if it is a maximum point. &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Figure 2: Contour plot of system displaced from transtition state. Calculation type: Dynamics]]&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 3: Contour plot of system displaced from transtion state. Calculation type: MEP|left]]&lt;br /&gt;
The minimum energy path or mep is take a path through the potential surface where it does not&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809109</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=809109"/>
		<updated>2020-05-21T21:11:38Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by mapping trajectories near the supposed transition state, and observe whether the line goes towards the products or reactants. Enough attempts will lead to an estimate of it, and it can be distinguished from a local minimum by finding &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Figure 2: Countour plot of system displaced from transtition state. Calculation type: Dynamics]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 2: Contour plot of system displaced from transtion state. Calculation type: MEP|left]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
Placeholder&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=808989</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=808989"/>
		<updated>2020-05-21T19:43:33Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph (&#039;&#039;&#039;Figure 1&#039;&#039;&#039;), it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Figure 2: Countour plot of system displaced from transtition state. Calculation type: Dynamics]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Figure 2: Contour plot of system displaced from transtion state. Calculation type: MEP|left]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
Placeholder&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=808985</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=808985"/>
		<updated>2020-05-21T19:42:44Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Comment on how the mep and the trajectory you just calculated differ */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph, it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Figure 2: Countour plot of system displaced from transtition state. Calculation type: Dynamics]][[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Contour plot of system displaced from transtion state. Calculation type: MEP|left]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
Placeholder&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=808981</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=808981"/>
		<updated>2020-05-21T19:42:18Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Comment on how the mep and the trajectory you just calculated differ */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Figure 1: Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|thumb|Contour plot of system displaced from transtion state. Calculation type: MEP]]&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by &lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph, it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Figure 2: Countour plot of system displaced from transtition state. Calculation type: Dynamics]]&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
Placeholder&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=808975</id>
		<title>MRD:01535442</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:01535442&amp;diff=808975"/>
		<updated>2020-05-21T19:39:39Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: /* Comment on how the mep and the trajectory you just calculated differ */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== Molecular Reaction Dynamics: Applications to Triatomic systems ==&lt;br /&gt;
In this report, we will be investigating the reaction dynamics of two triatomic systems, H-H-H and F-H-H. This includes investigation of their transition states, reaction coordinates and potential energy surfaces, and how these affect the outcome of chemical reactions.&lt;br /&gt;
&lt;br /&gt;
== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; System ==&lt;br /&gt;
&lt;br /&gt;
=== On a potential energy surface diagram, how is the transition state mathematically defined? ===&lt;br /&gt;
∂V(&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;)/∂&#039;&#039;&#039;r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&#039;=0 defines the point in the potential enrgy surface diagram where to gradient is zero, being defined as the maximum on the minimum energy curve.&lt;br /&gt;
&lt;br /&gt;
=== How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface? ===&lt;br /&gt;
The transitions state can be identified by &lt;br /&gt;
[[File:Internuclear Dist vs Time for rts 1535442.png|thumb|Internuclear Distance vs Time Graph for H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system, best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
=== Report your best estimate of the transition state position (&#039;&#039;&#039;r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;&#039;&#039;&#039;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory ===&lt;br /&gt;
The best estimate for r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; (the transition state position) is 90.8 pm. If you take a look at the internuclear distance vs time graph, it shows that across time, there is no oscillatory behaviour in the triatomic system that alters the distance from the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;, therefore 90.8 pm is the closest estimate for this position. Note that distance A-B and B-C are the same, so line A-B in the graph is behind line B-C.&lt;br /&gt;
&lt;br /&gt;
=== Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ ===&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts Dynamics 01535442.png|left|thumb|Countour plot of system slighlty displaced from transtition state position. Calculation type:Dynamics]]Placeholder&lt;br /&gt;
&lt;br /&gt;
[[File:Contour Plot of Rts +1, Rts MEP 01535442.png|left|thumb|Contour plot of system slightly displaced from transtion state position. Calculation type:MEP]]&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_Rts_%2B1,_Rts_MEP_01535442.png&amp;diff=808974</id>
		<title>File:Contour Plot of Rts +1, Rts MEP 01535442.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Plot_of_Rts_%2B1,_Rts_MEP_01535442.png&amp;diff=808974"/>
		<updated>2020-05-21T19:37:52Z</updated>

		<summary type="html">&lt;p&gt;Tr1318: Contour plot of a system with slighlty displaced transtition state position, calculated using MEP (minimum energy path).&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Contour plot of a system with slighlty displaced transtition state position, calculated using MEP (minimum energy path).&lt;/div&gt;</summary>
		<author><name>Tr1318</name></author>
	</entry>
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