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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=808168</id>
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		<summary type="html">&lt;p&gt;Jy8418: /* Answer 1: */&lt;/p&gt;
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== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms (in a symmetric case), the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on LHS and products on RHS). &lt;br /&gt;
[[File:exo0.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 160 pm, momentum is p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the momentum p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is tested in range between -6.7 to 6.7 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Under such high vibrational energy, it is hard to obtain a reactive trajectory, so reaction 1 is inefficient at a high vibrational energy and a low translational energy. However, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is reduced to 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; slightly increased to -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, a reactive trajectory is obtained. Therefore, in case of a high portion of translational energy and a low vibrational energy, reaction is efficient.&lt;br /&gt;
&lt;br /&gt;
For reaction 2--HF+H, the same procedure is repeated. This time, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 60 pm. At high translational energy (high p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;) and low vibrational energy (low p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;), it is hard to obtain a reactive trajectory. When a high vibrational energy and a low translational energy is set, a reactive trajectory is obtained. (e.g. p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-5.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;,p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1.0 g.mol-1.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;) Therefore, reaction 2 is efficient under a high portion of vibrational energy and a low translational energy.&lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s empirical rule, high translational energy would be more effective for reactions with an early transition state than vibrational energy; vice versa for reactions with a late transition state. This theory is supported by experimental results. Figure 10 shows the energy pathway for reaction 1. Its transition state is closer to the reactants (LHS), so it is an early transition state. Owing to this early transition state, reaction 1 is efficient when a large portion of translational energy is applied.  Figure 11 shows the energy pathway for reaction 2. Its transition state is closer to the products H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(RHS), so it is a late transition state. Owing to this late transition state, reaction 2 is more efficient when a large portion of vibrational energy is applied. All the experimental results fit the theory.&lt;br /&gt;
&lt;br /&gt;
[[File:early.png|thumb|frame|left|Figure 10-energy pathway for reaction 1]]&lt;br /&gt;
[[File:late.png|thumb|none|Figure 11-energy pathway for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
1.Yabushita, Satoshi. “Relativistic Effects on Transition State Structures and Properties: Transition State Spectroscopy of IHI and BrHI.” &#039;&#039;The Transition State&#039;&#039;, 2019, pp. 267–282., doi:10.1201/9780367810573-13.&lt;br /&gt;
&lt;br /&gt;
2.Polanyi, J. C., and D. C. Tardy. “Energy Distribution in the Exothermic Reaction F   H2 and the Endothermic Reaction HF   H.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 51, no. 12, 1969, pp. 5717–5719., doi:10.1063/1.1672005.&lt;br /&gt;
&lt;br /&gt;
3.Guo, Hua, and Kopin Liu. “ChemInform Abstract: Control of Chemical Reactivity by Transition-State and Beyond.” &#039;&#039;ChemInform&#039;&#039;, vol. 47, no. 33, 2016, doi:10.1002/chin.201633256.&lt;br /&gt;
&lt;br /&gt;
4.Zhao, Bin, et al. “Communication: State-to-State Dynamics of the Cl H2O → HCl OH Reaction: Energy Flow into Reaction Coordinate and Transition-State Control of Product Energy Disposal.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 142, no. 24, 2015, p. 241101., doi:10.1063/1.4922650.&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=807004</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=807004"/>
		<updated>2020-05-20T01:59:40Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 10: */&lt;/p&gt;
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&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on LHS and products on RHS). &lt;br /&gt;
[[File:exo0.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 160 pm, momentum is p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the momentum p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is tested in range between -6.7 to 6.7 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Under such high vibrational energy, it is hard to obtain a reactive trajectory, so reaction 1 is inefficient at a high vibrational energy and a low translational energy. However, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is reduced to 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; slightly increased to -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, a reactive trajectory is obtained. Therefore, in case of a high portion of translational energy and a low vibrational energy, reaction is efficient.&lt;br /&gt;
&lt;br /&gt;
For reaction 2--HF+H, the same procedure is repeated. This time, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 60 pm. At high translational energy (high p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;) and low vibrational energy (low p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;), it is hard to obtain a reactive trajectory. When a high vibrational energy and a low translational energy is set, a reactive trajectory is obtained. (e.g. p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-5.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;,p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1.0 g.mol-1.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;) Therefore, reaction 2 is efficient under a high portion of vibrational energy and a low translational energy.&lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s empirical rule, high translational energy would be more effective for reactions with an early transition state than vibrational energy; vice versa for reactions with a late transition state. This theory is supported by experimental results. Figure 10 shows the energy pathway for reaction 1. Its transition state is closer to the reactants (LHS), so it is an early transition state. Owing to this early transition state, reaction 1 is efficient when a large portion of translational energy is applied.  Figure 11 shows the energy pathway for reaction 2. Its transition state is closer to the products H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(RHS), so it is a late transition state. Owing to this late transition state, reaction 2 is more efficient when a large portion of vibrational energy is applied. All the experimental results fit the theory.&lt;br /&gt;
&lt;br /&gt;
[[File:early.png|thumb|frame|left|Figure 10-energy pathway for reaction 1]]&lt;br /&gt;
[[File:late.png|thumb|none|Figure 11-energy pathway for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
1.Yabushita, Satoshi. “Relativistic Effects on Transition State Structures and Properties: Transition State Spectroscopy of IHI and BrHI.” &#039;&#039;The Transition State&#039;&#039;, 2019, pp. 267–282., doi:10.1201/9780367810573-13.&lt;br /&gt;
&lt;br /&gt;
2.Polanyi, J. C., and D. C. Tardy. “Energy Distribution in the Exothermic Reaction F   H2 and the Endothermic Reaction HF   H.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 51, no. 12, 1969, pp. 5717–5719., doi:10.1063/1.1672005.&lt;br /&gt;
&lt;br /&gt;
3.Guo, Hua, and Kopin Liu. “ChemInform Abstract: Control of Chemical Reactivity by Transition-State and Beyond.” &#039;&#039;ChemInform&#039;&#039;, vol. 47, no. 33, 2016, doi:10.1002/chin.201633256.&lt;br /&gt;
&lt;br /&gt;
4.Zhao, Bin, et al. “Communication: State-to-State Dynamics of the Cl H2O → HCl OH Reaction: Energy Flow into Reaction Coordinate and Transition-State Control of Product Energy Disposal.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 142, no. 24, 2015, p. 241101., doi:10.1063/1.4922650.&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=807003</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=807003"/>
		<updated>2020-05-20T01:59:13Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 10: */&lt;/p&gt;
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&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on LHS and products on RHS). &lt;br /&gt;
[[File:exo0.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 160 pm, momentum is p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the momentum p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is tested in range between -6.7 to 6.7 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Under such high vibrational energy, it is hard to obtain a reactive trajectory, so reaction 1 is inefficient at a high vibrational energy and a low translational energy. However, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is reduced to 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; slightly increased to -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, a reactive trajectory is obtained. Therefore, in case of a high portion of translational energy and a low vibrational energy, reaction is efficient.&lt;br /&gt;
&lt;br /&gt;
For reaction 2--HF+H, the same procedure is repeated. This time, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 60 pm. At high translational energy (high p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;) and low vibrational energy (low p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;), it is hard to obtain a reactive trajectory. When a high vibrational energy and a low translational energy is set, a reactive trajectory is obtained. (e.g. p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-5.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;,p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1.0 g.mol-1.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;) Therefore, reaction 2 is efficient under a high portion of vibrational energy and a low translational energy.&lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s empirical rule, high translational energy would be more effective for reactions with an early transition state than vibrational energy; vice versa for reactions with a late transition state. This theory is supported by experimental results. Figure 10 shows the energy pathway for reaction 1. Its transition state is closer to the reactants (LHS), so it is an early transition state. Owing to this early transition state, reaction 1 is efficient when a large portion of translational energy is applied.  Figure 11 shows the energy pathway for reaction 2. Its transition state is closer to the products H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(RHS), so it is a late transition state. Owing to this late transition state, reaction 2 is more efficient when a large portion of vibrational energy is applied. All the experimental results fit the theory.&lt;br /&gt;
&lt;br /&gt;
[[File:early.png|thumb|frame|left|Figure 10-energy pathway for reaction 1]]&lt;br /&gt;
[[File:late.png|thumb|right|Figure 11-energy pathway for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
1.Yabushita, Satoshi. “Relativistic Effects on Transition State Structures and Properties: Transition State Spectroscopy of IHI and BrHI.” &#039;&#039;The Transition State&#039;&#039;, 2019, pp. 267–282., doi:10.1201/9780367810573-13.&lt;br /&gt;
&lt;br /&gt;
2.Polanyi, J. C., and D. C. Tardy. “Energy Distribution in the Exothermic Reaction F   H2 and the Endothermic Reaction HF   H.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 51, no. 12, 1969, pp. 5717–5719., doi:10.1063/1.1672005.&lt;br /&gt;
&lt;br /&gt;
3.Guo, Hua, and Kopin Liu. “ChemInform Abstract: Control of Chemical Reactivity by Transition-State and Beyond.” &#039;&#039;ChemInform&#039;&#039;, vol. 47, no. 33, 2016, doi:10.1002/chin.201633256.&lt;br /&gt;
&lt;br /&gt;
4.Zhao, Bin, et al. “Communication: State-to-State Dynamics of the Cl H2O → HCl OH Reaction: Energy Flow into Reaction Coordinate and Transition-State Control of Product Energy Disposal.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 142, no. 24, 2015, p. 241101., doi:10.1063/1.4922650.&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=807002</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=807002"/>
		<updated>2020-05-20T01:58:18Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 10: */&lt;/p&gt;
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&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on LHS and products on RHS). &lt;br /&gt;
[[File:exo0.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 160 pm, momentum is p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the momentum p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is tested in range between -6.7 to 6.7 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Under such high vibrational energy, it is hard to obtain a reactive trajectory, so reaction 1 is inefficient at a high vibrational energy and a low translational energy. However, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is reduced to 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; slightly increased to -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, a reactive trajectory is obtained. Therefore, in case of a high portion of translational energy and a low vibrational energy, reaction is efficient.&lt;br /&gt;
&lt;br /&gt;
For reaction 2--HF+H, the same procedure is repeated. This time, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 60 pm. At high translational energy (high p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;) and low vibrational energy (low p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;), it is hard to obtain a reactive trajectory. When a high vibrational energy and a low translational energy is set, a reactive trajectory is obtained. (e.g. p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-5.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;,p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1.0 g.mol-1.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;) Therefore, reaction 2 is efficient under a high portion of vibrational energy and a low translational energy.&lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s empirical rule, high translational energy would be more effective for reactions with an early transition state than vibrational energy; vice versa for reactions with a late transition state. This theory is supported by experimental results. Figure 10 shows the energy pathway for reaction 1. Its transition state is closer to the reactants (LHS), so it is an early transition state. Owing to this early transition state, reaction 1 is efficient when a large portion of translational energy is applied.  Figure 11 shows the energy pathway for reaction 2. Its transition state is closer to the products H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(RHS), so it is a late transition state. Owing to this late transition state, reaction 2 is more efficient when a large portion of vibrational energy is applied. All the experimental results fit the theory.&lt;br /&gt;
&lt;br /&gt;
[[File:early.png|thumb|frame|left|Figure 10-energy pathway for reaction 1]]&lt;br /&gt;
[[File:late.png|thumb|none|Figure 11-energy pathway for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
1.Yabushita, Satoshi. “Relativistic Effects on Transition State Structures and Properties: Transition State Spectroscopy of IHI and BrHI.” &#039;&#039;The Transition State&#039;&#039;, 2019, pp. 267–282., doi:10.1201/9780367810573-13.&lt;br /&gt;
&lt;br /&gt;
2.Polanyi, J. C., and D. C. Tardy. “Energy Distribution in the Exothermic Reaction F   H2 and the Endothermic Reaction HF   H.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 51, no. 12, 1969, pp. 5717–5719., doi:10.1063/1.1672005.&lt;br /&gt;
&lt;br /&gt;
3.Guo, Hua, and Kopin Liu. “ChemInform Abstract: Control of Chemical Reactivity by Transition-State and Beyond.” &#039;&#039;ChemInform&#039;&#039;, vol. 47, no. 33, 2016, doi:10.1002/chin.201633256.&lt;br /&gt;
&lt;br /&gt;
4.Zhao, Bin, et al. “Communication: State-to-State Dynamics of the Cl H2O → HCl OH Reaction: Energy Flow into Reaction Coordinate and Transition-State Control of Product Energy Disposal.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 142, no. 24, 2015, p. 241101., doi:10.1063/1.4922650.&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=807000</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=807000"/>
		<updated>2020-05-20T01:51:27Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 10: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on LHS and products on RHS). &lt;br /&gt;
[[File:exo0.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 160 pm, momentum is p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the momentum p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is tested in range between -6.7 to 6.7 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Under such high vibrational energy, it is hard to obtain a reactive trajectory, so reaction 1 is inefficient at a high vibrational energy and a low translational energy. However, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is reduced to 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; slightly increased to -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, a reactive trajectory is obtained. Therefore, in case of a high portion of translational energy and a low vibrational energy, reaction is efficient.&lt;br /&gt;
&lt;br /&gt;
For reaction 2--HF+H, the same procedure is repeated. This time, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 60 pm. At high translational energy (high p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;) and low vibrational energy (low p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;), it is hard to obtain a reactive trajectory. When a high vibrational energy and a low translational energy is set, a reactive trajectory is obtained. (e.g. p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-5.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;,p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1.0 g.mol-1.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;) Therefore, reaction 2 is efficient under a high portion of vibrational energy and a low translational energy.&lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s empirical rule, high translational energy would be more effective for reactions with an early transition state than vibrational energy; vice versa for reactions with a late transition state. This theory is supported by experimental results. Figure 10 shows the energy pathway for reaction 1. Its transition state is closer to the reactants (LHS), so it is an early transition state. Owing to this early transition state, reaction 1 is efficient when a large portion of translational energy is applied.  Figure 11 shows the energy pathway for reaction 2. Its transition state is closer to the products H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(RHS), so it is a late transition state. Owing to this late transition state, reaction 2 is more efficient when a large portion of vibrational energy is applied. All the experimental results fit the theory.&lt;br /&gt;
&lt;br /&gt;
[[File:early.png|thumb|frame|left|Figure 10-energy pathway for reaction 1]]&lt;br /&gt;
[[File:late.png|thumb|none|Figure 11-energy pathway for reaction 2|231x231px]]&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
1.Yabushita, Satoshi. “Relativistic Effects on Transition State Structures and Properties: Transition State Spectroscopy of IHI and BrHI.” &#039;&#039;The Transition State&#039;&#039;, 2019, pp. 267–282., doi:10.1201/9780367810573-13.&lt;br /&gt;
&lt;br /&gt;
2.Polanyi, J. C., and D. C. Tardy. “Energy Distribution in the Exothermic Reaction F   H2 and the Endothermic Reaction HF   H.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 51, no. 12, 1969, pp. 5717–5719., doi:10.1063/1.1672005.&lt;br /&gt;
&lt;br /&gt;
3.Guo, Hua, and Kopin Liu. “ChemInform Abstract: Control of Chemical Reactivity by Transition-State and Beyond.” &#039;&#039;ChemInform&#039;&#039;, vol. 47, no. 33, 2016, doi:10.1002/chin.201633256.&lt;br /&gt;
&lt;br /&gt;
4.Zhao, Bin, et al. “Communication: State-to-State Dynamics of the Cl H2O → HCl OH Reaction: Energy Flow into Reaction Coordinate and Transition-State Control of Product Energy Disposal.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 142, no. 24, 2015, p. 241101., doi:10.1063/1.4922650.&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806579</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806579"/>
		<updated>2020-05-19T13:56:44Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on LHS and products on RHS). &lt;br /&gt;
[[File:exo0.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 160 pm, momentum is p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the momentum p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is tested in range between -6.7 to 6.7 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Under such high vibrational energy, it is hard to obtain a reactive trajectory, so reaction 1 is inefficient at a high vibrational energy and a low translational energy. However, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is reduced to 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; slightly increased to -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, a reactive trajectory is obtained. Therefore, in case of a high portion of translational energy and a low vibrational energy, reaction is efficient.&lt;br /&gt;
&lt;br /&gt;
For reaction 2--HF+H, the same procedure is repeated. This time, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 60 pm. At high translational energy (high p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;) and low vibrational energy (low p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;), it is hard to obtain a reactive trajectory. When a high vibrational energy and a low translational energy is set, a reactive trajectory is obtained. (e.g. p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-5.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;,p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1.0 g.mol-1.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;) Therefore, reaction 2 is efficient under a high portion of vibrational energy and a low translational energy.&lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s empirical rule, high translational energy would be more effective for reactions with an early transition state than vibrational energy; vice versa for reactions with a late transition state. This theory is supported by experimental results. Figure 10 shows the energy pathway for reaction 1. Its transition state is closer to the reactants (LHS), so it is an early transition state. Owing to this early transition state, reaction 1 is efficient when a large portion of translational energy is applied.  Figure 11 shows the energy pathway for reaction 2. Its transition state is closer to the products H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(RHS), so it is a late transition state. Owing to this late transition state, reaction 2 is more efficient when a large portion of vibrational energy is applied. All the experimental results fit the theory.&lt;br /&gt;
&lt;br /&gt;
[[File:early.png|thumb|frame|left|Figure 10-energy pathway for reaction 1]]&lt;br /&gt;
[[File:late.png|thumb|none|Figure 11-energy pathway for reaction 2|221x221px]]&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
1.Yabushita, Satoshi. “Relativistic Effects on Transition State Structures and Properties: Transition State Spectroscopy of IHI and BrHI.” &#039;&#039;The Transition State&#039;&#039;, 2019, pp. 267–282., doi:10.1201/9780367810573-13.&lt;br /&gt;
&lt;br /&gt;
2.Polanyi, J. C., and D. C. Tardy. “Energy Distribution in the Exothermic Reaction F   H2 and the Endothermic Reaction HF   H.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 51, no. 12, 1969, pp. 5717–5719., doi:10.1063/1.1672005.&lt;br /&gt;
&lt;br /&gt;
3.Guo, Hua, and Kopin Liu. “ChemInform Abstract: Control of Chemical Reactivity by Transition-State and Beyond.” &#039;&#039;ChemInform&#039;&#039;, vol. 47, no. 33, 2016, doi:10.1002/chin.201633256.&lt;br /&gt;
&lt;br /&gt;
4.Zhao, Bin, et al. “Communication: State-to-State Dynamics of the Cl H2O → HCl OH Reaction: Energy Flow into Reaction Coordinate and Transition-State Control of Product Energy Disposal.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 142, no. 24, 2015, p. 241101., doi:10.1063/1.4922650.&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806560</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806560"/>
		<updated>2020-05-19T13:51:07Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 10: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on LHS and products on RHS). &lt;br /&gt;
[[File:exo0.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 160 pm, momentum is p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the momentum p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is tested in range between -6.7 to 6.7 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Under such high vibrational energy, it is hard to obtain a reactive trajectory, so reaction 1 is inefficient at a high vibrational energy and a low translational energy. However, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is reduced to 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; slightly increased to -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, a reactive trajectory is obtained. Therefore, in case of a high portion of translational energy and a low vibrational energy, reaction is efficient.&lt;br /&gt;
&lt;br /&gt;
For reaction 2--HF+H, the same procedure is repeated. This time, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 60 pm. At high translational energy (high p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;) and low vibrational energy (low p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;), it is hard to obtain a reactive trajectory. When a high vibrational energy and a low translational energy is set, a reactive trajectory is obtained. (e.g. p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-5.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;,p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1.0 g.mol-1.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;) Therefore, reaction 2 is efficient under a high portion of vibrational energy and a low translational energy.&lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s empirical rule, high translational energy would be more effective for reactions with an early transition state than vibrational energy; vice versa for reactions with a late transition state. This theory is supported by experimental results. Figure 10 shows the energy pathway for reaction 1. Its transition state is closer to the reactants (LHS), so it is an early transition state. Owing to this early transition state, reaction 1 is efficient when a large portion of translational energy is applied.  Figure 11 shows the energy pathway for reaction 2. Its transition state is closer to the products H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(RHS), so it is a late transition state. Owing to this late transition state, reaction 2 is more efficient when a large portion of vibrational energy is applied. All the experimental results fit the theory.&lt;br /&gt;
&lt;br /&gt;
[[File:early.png|thumb|frame|left|Figure 10-energy pathway for reaction 1]]&lt;br /&gt;
[[File:late.png|thumb|frame|none|Figure 11-energy pathway for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
1.Yabushita, Satoshi. “Relativistic Effects on Transition State Structures and Properties: Transition State Spectroscopy of IHI and BrHI.” &#039;&#039;The Transition State&#039;&#039;, 2019, pp. 267–282., doi:10.1201/9780367810573-13.&lt;br /&gt;
&lt;br /&gt;
2.Polanyi, J. C., and D. C. Tardy. “Energy Distribution in the Exothermic Reaction F   H2 and the Endothermic Reaction HF   H.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 51, no. 12, 1969, pp. 5717–5719., doi:10.1063/1.1672005.&lt;br /&gt;
&lt;br /&gt;
3.Guo, Hua, and Kopin Liu. “ChemInform Abstract: Control of Chemical Reactivity by Transition-State and Beyond.” &#039;&#039;ChemInform&#039;&#039;, vol. 47, no. 33, 2016, doi:10.1002/chin.201633256.&lt;br /&gt;
&lt;br /&gt;
4.Zhao, Bin, et al. “Communication: State-to-State Dynamics of the Cl H2O → HCl OH Reaction: Energy Flow into Reaction Coordinate and Transition-State Control of Product Energy Disposal.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 142, no. 24, 2015, p. 241101., doi:10.1063/1.4922650.&lt;/div&gt;</summary>
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== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on LHS and products on RHS). &lt;br /&gt;
[[File:exo0.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 160 pm, momentum is p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, the momentum p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is tested in range between -6.7 to 6.7 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. Under such high vibrational energy, it is hard to obtain a reactive trajectory, so reaction 1 is inefficient at a high vibrational energy and a low translational energy. However, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is reduced to 0.2 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; slightly increased to -1.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, a reactive trajectory is obtained. Therefore, in case of a high portion of translational energy and a low vibrational energy, reaction is efficient.&lt;br /&gt;
&lt;br /&gt;
For reaction 2--HF+H, the same procedure is repeated. This time, the positions are set at r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 60 pm. At high translational energy (high p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;) and low vibrational energy (low p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;), it is hard to obtain a reactive trajectory. When a high vibrational energy and a low translational energy is set, a reactive trajectory is obtained. (e.g. p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-5.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;,p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1.0 g.mol-1.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;) Therefore, reaction 2 is efficient under a high portion of vibrational energy and a low translational energy.&lt;br /&gt;
&lt;br /&gt;
According to Polanyi&#039;s empirical rule, high translational energy would be more effective for reactions with an early transition state than vibrational energy; vice versa for reactions with a late transition state. This theory is supported by experimental results. Figure 10 shows the energy pathway for reaction 1. Its transition state is closer to the reactants (LHS), so it is an early transition state. Owing to this early transition state, reaction 1 is efficient when a large portion of translational energy is applied.  Figure 11 shows the energy pathway for reaction 2. Its transition state is closer to the products H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;(RHS), so it is a late transition state. Owing to this late transition state, reaction 2 is more efficient when a large portion of vibrational energy is applied. All the experimental results fit the theory.&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
1.Yabushita, Satoshi. “Relativistic Effects on Transition State Structures and Properties: Transition State Spectroscopy of IHI and BrHI.” &#039;&#039;The Transition State&#039;&#039;, 2019, pp. 267–282., doi:10.1201/9780367810573-13.&lt;br /&gt;
&lt;br /&gt;
2.Polanyi, J. C., and D. C. Tardy. “Energy Distribution in the Exothermic Reaction F   H2 and the Endothermic Reaction HF   H.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 51, no. 12, 1969, pp. 5717–5719., doi:10.1063/1.1672005.&lt;br /&gt;
&lt;br /&gt;
3.Guo, Hua, and Kopin Liu. “ChemInform Abstract: Control of Chemical Reactivity by Transition-State and Beyond.” &#039;&#039;ChemInform&#039;&#039;, vol. 47, no. 33, 2016, doi:10.1002/chin.201633256.&lt;br /&gt;
&lt;br /&gt;
4.Zhao, Bin, et al. “Communication: State-to-State Dynamics of the Cl H2O → HCl OH Reaction: Energy Flow into Reaction Coordinate and Transition-State Control of Product Energy Disposal.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 142, no. 24, 2015, p. 241101., doi:10.1063/1.4922650.&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806254</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806254"/>
		<updated>2020-05-19T08:46:05Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on LHS and products on RHS). &lt;br /&gt;
[[File:exo0.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=8 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 10) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:1vibb.png|thumb|frame|none|Figure 10-The trajectory for reaction 1 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-14.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 11) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:1trans.png|thumb|frame|none|Figure 11-The trajectory for reaction 1 under high translational energy]]&lt;br /&gt;
For reaction 2--HF+H, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-12.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 12) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:2vibb.png|thumb|frame|none|Figure 12-The trajectory for reaction 2 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-9.8 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;a reactive trajectory (Figure 13) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:2trans.png|thumb|frame|none|Figure 13-The trajectory for reaction 2 under high translational energy]]&lt;br /&gt;
Therefore, high vibrational energy and low translational energy indicate the presence the early transition state; high translational energy and low vibrational energy favour the late transition state.&lt;br /&gt;
&lt;br /&gt;
When investigating for the reactive trajectories, it is found that if the vibrational energy is high, the reaction can be more efficient (early transition state). According to Polanyi&#039;s principle,&lt;br /&gt;
&lt;br /&gt;
E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;=E&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;+αΔH&lt;br /&gt;
&lt;br /&gt;
where E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; is the activation energy, α is the position of transition state along the reaction coordinates. An early transition state (at high vibrational energy) indicates a small value of α, thus lower activation energy, making the reaction more efficient.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;*&amp;lt;/nowiki&amp;gt;In all figures 10-13, the reactants are on LHS and products on RHS.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
1.Yabushita, Satoshi. “Relativistic Effects on Transition State Structures and Properties: Transition State Spectroscopy of IHI and BrHI.” &#039;&#039;The Transition State&#039;&#039;, 2019, pp. 267–282., doi:10.1201/9780367810573-13.&lt;br /&gt;
&lt;br /&gt;
2.Polanyi, J. C., and D. C. Tardy. “Energy Distribution in the Exothermic Reaction F   H2 and the Endothermic Reaction HF   H.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 51, no. 12, 1969, pp. 5717–5719., doi:10.1063/1.1672005.&lt;br /&gt;
&lt;br /&gt;
3.Guo, Hua, and Kopin Liu. “ChemInform Abstract: Control of Chemical Reactivity by Transition-State and Beyond.” &#039;&#039;ChemInform&#039;&#039;, vol. 47, no. 33, 2016, doi:10.1002/chin.201633256.&lt;br /&gt;
&lt;br /&gt;
4.Zhao, Bin, et al. “Communication: State-to-State Dynamics of the Cl H2O → HCl OH Reaction: Energy Flow into Reaction Coordinate and Transition-State Control of Product Energy Disposal.” &#039;&#039;The Journal of Chemical Physics&#039;&#039;, vol. 142, no. 24, 2015, p. 241101., doi:10.1063/1.4922650.&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806253</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806253"/>
		<updated>2020-05-19T03:29:00Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 10: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on LHS and products on RHS). &lt;br /&gt;
[[File:exo0.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=8 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 10) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:1vibb.png|thumb|frame|none|Figure 10-The trajectory for reaction 1 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-14.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 11) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:1trans.png|thumb|frame|none|Figure 11-The trajectory for reaction 1 under high translational energy]]&lt;br /&gt;
For reaction 2--HF+H, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-12.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 12) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:2vibb.png|thumb|frame|none|Figure 12-The trajectory for reaction 2 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-9.8 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;a reactive trajectory (Figure 13) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:2trans.png|thumb|frame|none|Figure 13-The trajectory for reaction 2 under high translational energy]]&lt;br /&gt;
Therefore, high vibrational energy and low translational energy indicate the presence the early transition state; high translational energy and low vibrational energy favour the late transition state.&lt;br /&gt;
&lt;br /&gt;
When investigating for the reactive trajectories, it is found that if the vibrational energy is high, the reaction can be more efficient (early transition state). According to Polanyi&#039;s principle,&lt;br /&gt;
&lt;br /&gt;
E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;=E&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;+αΔH&lt;br /&gt;
&lt;br /&gt;
where E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; is the activation energy, α is the position of transition state along the reaction coordinates. An early transition state (at high vibrational energy) indicates a small value of α, thus lower activation energy, making the reaction more efficient.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;*&amp;lt;/nowiki&amp;gt;In all figures 10-13, the reactants are on LHS and products on RHS.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://pubs.rsc.org/en/content/articlehtml/2016/sc/c6sc01066k&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806252</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806252"/>
		<updated>2020-05-19T03:22:52Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 6: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on LHS and products on RHS). &lt;br /&gt;
[[File:exo0.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=8 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 10) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:1vibb.png|thumb|frame|none|Figure 10-The trajectory for reaction 1 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-14.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 11) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:1trans.png|thumb|frame|none|Figure 11-The trajectory for reaction 1 under high translational energy]]&lt;br /&gt;
For reaction 2--HF+H, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-12.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 12) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:2vibb.png|thumb|frame|none|Figure 12-The trajectory for reaction 2 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-9.8 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;a reactive trajectory (Figure 13) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:2trans.png|thumb|frame|none|Figure 13-The trajectory for reaction 2 under high translational energy]]&lt;br /&gt;
Therefore, high vibrational energy and low translational energy indicate the presence the early transition state; high translational energy and low vibrational energy favour the late transition state.&lt;br /&gt;
&lt;br /&gt;
When investigating for the reactive trajectories, it is found that if the vibrational energy is high, the reaction can be more efficient (early transition state). According to Polanyi&#039;s principle,&lt;br /&gt;
&lt;br /&gt;
E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;=E&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;+αΔH&lt;br /&gt;
&lt;br /&gt;
where E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; is the activation energy, α is the position of transition state along the reaction coordinates. An early transition state (at high vibrational energy) indicates a small value of α, thus lower activation energy, making the reaction more efficient.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;*&amp;lt;/nowiki&amp;gt;In figures 10-11, the reactants are on RHS and products on LHS; for figures 12-13, the reactants are on LHS and products on RHS.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://pubs.rsc.org/en/content/articlehtml/2016/sc/c6sc01066k&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806251</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806251"/>
		<updated>2020-05-19T03:21:06Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 6: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on LHS and products on RHS). &lt;br /&gt;
[[File:exo0.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (more negative in value) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=8 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 10) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:1vibb.png|thumb|frame|none|Figure 10-The trajectory for reaction 1 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-14.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 11) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:1trans.png|thumb|frame|none|Figure 11-The trajectory for reaction 1 under high translational energy]]&lt;br /&gt;
For reaction 2--HF+H, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-12.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 12) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:2vibb.png|thumb|frame|none|Figure 12-The trajectory for reaction 2 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-9.8 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;a reactive trajectory (Figure 13) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:2trans.png|thumb|frame|none|Figure 13-The trajectory for reaction 2 under high translational energy]]&lt;br /&gt;
Therefore, high vibrational energy and low translational energy indicate the presence the early transition state; high translational energy and low vibrational energy favour the late transition state.&lt;br /&gt;
&lt;br /&gt;
When investigating for the reactive trajectories, it is found that if the vibrational energy is high, the reaction can be more efficient (early transition state). According to Polanyi&#039;s principle,&lt;br /&gt;
&lt;br /&gt;
E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;=E&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;+αΔH&lt;br /&gt;
&lt;br /&gt;
where E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; is the activation energy, α is the position of transition state along the reaction coordinates. An early transition state (at high vibrational energy) indicates a small value of α, thus lower activation energy, making the reaction more efficient.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;*&amp;lt;/nowiki&amp;gt;In figures 10-11, the reactants are on RHS and products on LHS; for figures 12-13, the reactants are on LHS and products on RHS.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://pubs.rsc.org/en/content/articlehtml/2016/sc/c6sc01066k&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Exo0.png&amp;diff=806250</id>
		<title>File:Exo0.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Exo0.png&amp;diff=806250"/>
		<updated>2020-05-19T03:19:23Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: &lt;/p&gt;
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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806249</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806249"/>
		<updated>2020-05-19T03:09:47Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* References */&lt;/p&gt;
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== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (more negative in value) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=8 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 10) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:1vibb.png|thumb|frame|none|Figure 10-The trajectory for reaction 1 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-14.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 11) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:1trans.png|thumb|frame|none|Figure 11-The trajectory for reaction 1 under high translational energy]]&lt;br /&gt;
For reaction 2--HF+H, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-12.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 12) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:2vibb.png|thumb|frame|none|Figure 12-The trajectory for reaction 2 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-9.8 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;a reactive trajectory (Figure 13) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:2trans.png|thumb|frame|none|Figure 13-The trajectory for reaction 2 under high translational energy]]&lt;br /&gt;
Therefore, high vibrational energy and low translational energy indicate the presence the early transition state; high translational energy and low vibrational energy favour the late transition state.&lt;br /&gt;
&lt;br /&gt;
When investigating for the reactive trajectories, it is found that if the vibrational energy is high, the reaction can be more efficient (early transition state). According to Polanyi&#039;s principle,&lt;br /&gt;
&lt;br /&gt;
E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;=E&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;+αΔH&lt;br /&gt;
&lt;br /&gt;
where E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; is the activation energy, α is the position of transition state along the reaction coordinates. An early transition state (at high vibrational energy) indicates a small value of α, thus lower activation energy, making the reaction more efficient.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;*&amp;lt;/nowiki&amp;gt;In figures 10-11, the reactants are on RHS and products on LHS; for figures 12-13, the reactants are on LHS and products on RHS.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://pubs.rsc.org/en/content/articlehtml/2016/sc/c6sc01066k&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806248</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806248"/>
		<updated>2020-05-19T02:43:47Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 10: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (more negative in value) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=8 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 10) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:1vibb.png|thumb|frame|none|Figure 10-The trajectory for reaction 1 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-14.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 11) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:1trans.png|thumb|frame|none|Figure 11-The trajectory for reaction 1 under high translational energy]]&lt;br /&gt;
For reaction 2--HF+H, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-12.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 12) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:2vibb.png|thumb|frame|none|Figure 12-The trajectory for reaction 2 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-9.8 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;a reactive trajectory (Figure 13) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:2trans.png|thumb|frame|none|Figure 13-The trajectory for reaction 2 under high translational energy]]&lt;br /&gt;
Therefore, high vibrational energy and low translational energy indicate the presence the early transition state; high translational energy and low vibrational energy favour the late transition state.&lt;br /&gt;
&lt;br /&gt;
When investigating for the reactive trajectories, it is found that if the vibrational energy is high, the reaction can be more efficient (early transition state). According to Polanyi&#039;s principle,&lt;br /&gt;
&lt;br /&gt;
E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;=E&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;+αΔH&lt;br /&gt;
&lt;br /&gt;
where E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; is the activation energy, α is the position of transition state along the reaction coordinates. An early transition state (at high vibrational energy) indicates a small value of α, thus lower activation energy, making the reaction more efficient.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;*&amp;lt;/nowiki&amp;gt;In figures 10-11, the reactants are on RHS and products on LHS; for figures 12-13, the reactants are on LHS and products on RHS.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806247</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806247"/>
		<updated>2020-05-19T02:32:43Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 10: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (more negative in value) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=8 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 10) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:1vibb.png|thumb|frame|none|Figure 10-The trajectory for reaction 1 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-14.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 11) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:1trans.png|thumb|frame|none|Figure 11-The trajectory for reaction 1 under high translational energy]]&lt;br /&gt;
For reaction 2--HF+H, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-12.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 12) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
[[File:2vibb.png|thumb|frame|none|Figure 12-The trajectory for reaction 2 under high vibrational energy]]&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-9.8 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;a reactive trajectory (Figure 13) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
[[File:2trans.png|thumb|frame|none|Figure 13-The trajectory for reaction 2 under high translational energy]]&lt;br /&gt;
Therefore, high vibrational energy and low translational energy indicate the presence the early transition state; high translational energy and low vibrational energy favour the late transition state.&lt;br /&gt;
&lt;br /&gt;
When investigating for the reactive trajectories, it is found that if the vibrational energy is high, the reaction can be more efficient (early transition state). According to Polanyi&#039;s principle,&lt;br /&gt;
&lt;br /&gt;
E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;=E&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;+αΔH&lt;br /&gt;
&lt;br /&gt;
where E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; is the activation energy, α is the position of transition state along the reaction coordinates. An early transition state (at high vibrational energy) indicates a small value of α, thus lower activation energy, making the reaction more efficient.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;*&amp;lt;/nowiki&amp;gt;In all the figures 10-13, the reactants are on LHS and products on RHS.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
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== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (more negative in value) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=8 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 10) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-14.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 11) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
&lt;br /&gt;
For reaction 2--HF+H, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-12.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 12) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-9.8 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;a reactive trajectory (Figure 13) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
&lt;br /&gt;
Therefore, high vibrational energy and low translational energy indicate the presence the early transition state; high translational energy and low vibrational energy favour the late transition state.&lt;br /&gt;
&lt;br /&gt;
When investigating for the reactive trajectories, it is found that if the vibrational energy is high, the reaction can be more efficient (early transition state). According to Polanyi&#039;s principle,&lt;br /&gt;
&lt;br /&gt;
E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;=E&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;+αΔH&lt;br /&gt;
&lt;br /&gt;
where E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt; is the activation energy, α is the position of transition state along the reaction coordinates. An early transition state (at high vibrational energy) indicates a small value of α, thus lower activation energy, making the reaction more efficient.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;*&amp;lt;/nowiki&amp;gt;In all the figures 10-13, the reactants are on LHS and products on RHS.&lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;References&#039;&#039;&#039; ==&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806165</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806165"/>
		<updated>2020-05-18T16:24:16Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 10: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (more negative in value) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
High vibrational energy and low translational energy favour the early transition state; high translational energy and low vibrational energy favour the late transition state. &lt;br /&gt;
&lt;br /&gt;
For all reactions, A B are the atoms in the molecule and C is the atom for colliding. When p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is set far more than p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; (p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high vibrational energy (and a low translational energy). Oppositely, when p&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;is set far less than pBC (p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is also given a low value), the system is said to have a high translational energy (and a low vibrational energy). &lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=8 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 10) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=74 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 182 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-14.6 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 11) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
&lt;br /&gt;
For reaction 2--HF+H, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-12.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1, &amp;lt;/sup&amp;gt;a reactive trajectory (Figure 12) is obtained. On the surface plot, at such high vibrational energy, the transition state was found closer to the reactants--early transition state.&lt;br /&gt;
&lt;br /&gt;
For the same reaction, when the positions are set at transition state of r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=182 pm and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;= 74 pm, p&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=-0.5 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=-9.8 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;a reactive trajectory (Figure 13) is obtained. On the surface plot, at such high translational energy, the transition state was found closer to the products--late transition state.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;*&amp;lt;/nowiki&amp;gt;In all the figures 10-13, the reactants are on LHS and products on RHS.&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806124</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806124"/>
		<updated>2020-05-17T15:22:54Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 9: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (more negative in value) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F, and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, based on the conservation of energy, the potential energy is converted to kinetic energy. The kinetic energy consists of vibrational and translational energy. The vibrational energy can be detected through infrared spectroscopy. To measure the heat change, a colorimeter can also be used to determine whether a reaction is endothermic or exothermic, by how much amount.&lt;br /&gt;
&lt;br /&gt;
==== Question 10 (Reaction dynamics): ====&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;
&lt;br /&gt;
==== Answer 10: ====&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806123</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806123"/>
		<updated>2020-05-17T08:12:55Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 9: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (more negative in value) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
The distance AB is set as 66 pm and distance BC is 210 pm. The momentum of AB is -9.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and that of C is -5.8 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;. Under this condition, the H&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;molecule vibrates towards F atom, after bouncing around a few times, the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; atom forms bonds with F and HF vibrates away.&lt;br /&gt;
&lt;br /&gt;
In this process, the potential energy is converted to kinetic energy.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806122</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806122"/>
		<updated>2020-05-17T07:57:57Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 8: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (more negative in value) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di8.png|thumb|frame|none|Figure 8-potential energy for the reactants 1]]&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:di9.png|thumb|frame|none|Figure 9-potential energy for the reactants 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
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== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the maximum (the one located at the least negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in a higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (more negative in value) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the transition state and the reactant. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7). For the potential energy of the reactants, it is assumed that the reactant species are not interacting, so the distance B-C is set near infinity and the most negative value of potential energy on the graph is taken as the potential energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants is -435.073 kJmol&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;(Figure 8), so the activation energy is 1.093 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
For reaction 2--HF+H, the potential energy for the reactants is -562.459 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;(Figure 9), so the activation energy is 127.386 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806118</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806118"/>
		<updated>2020-05-17T07:11:51Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 8: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold in Figure 1) linking reactants and reactants is plotted, the transition state is the minimum (the one located at the most negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in higher energy level than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the reactants and the transition state. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -433.980 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7).&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants&lt;br /&gt;
&lt;br /&gt;
==== Question 9 (Reaction dynamics): ====&lt;br /&gt;
In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.&lt;br /&gt;
&lt;br /&gt;
==== Answer 9: ====&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806117</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806117"/>
		<updated>2020-05-17T06:56:33Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 8: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold) linking reactants and reactants is plotted, the transition state is the minimum (the one located at the most negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in higher energy level (more negative in potential energy values) than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (less negative in potential energy values) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the reactants and the transition state. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -434.757 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7).&lt;br /&gt;
&lt;br /&gt;
[[File:tsenergy.png|thumb|frame|none|Figure 7-potential energy for the transition state]]&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Tsenergy.png&amp;diff=806116</id>
		<title>File:Tsenergy.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Tsenergy.png&amp;diff=806116"/>
		<updated>2020-05-17T06:53:25Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806115</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806115"/>
		<updated>2020-05-17T06:52:50Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 7: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold) linking reactants and reactants is plotted, the transition state is the minimum (the one located at the most negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in higher energy level (more negative in potential energy values) than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (less negative in potential energy values) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
==== Question 8 (PES inspection): ====&lt;br /&gt;
Report the activation energy for both reactions.&lt;br /&gt;
&lt;br /&gt;
==== Answer 8: ====&lt;br /&gt;
The activation energy is calculated as the difference between the potential energy of the reactants and the transition state. The respective energies are determined by plotting &amp;quot;Energy vs Time&amp;quot; graphs. As the transition state for both reactions are at the same position with the same structure of F--H--H, the two reactions have the same potential energy for the transition state, which is -434.757 kJmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (Figure 7).&lt;br /&gt;
&lt;br /&gt;
For reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the potential energy for the reactants&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806037</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806037"/>
		<updated>2020-05-16T09:51:40Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 7: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold) linking reactants and reactants is plotted, the transition state is the minimum (the one located at the most negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in higher energy level (more negative in potential energy values) than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (less negative in potential energy values) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|none|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|none|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806036</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806036"/>
		<updated>2020-05-16T09:50:14Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Question 1 (Dynamics from the transition state region): */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold) linking reactants and reactants is plotted, the transition state is the minimum (the one located at the most negative potential energy value). (Figure 1) On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in higher energy level (more negative in potential energy values) than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (less negative in potential energy values) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines (Figure 5 &amp;amp; 6). For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806034</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806034"/>
		<updated>2020-05-16T09:48:15Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold) linking reactants and reactants is plotted, the transition state is the minimum (the one located at the most negative potential energy value). On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|thumb|frame|right|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in higher energy level (more negative in potential energy values) than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (less negative in potential energy values) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines. For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806033</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806033"/>
		<updated>2020-05-16T09:47:12Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
[[File:path1.jpg|thumb|frame|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold) linking reactants and reactants is plotted, the transition state is the minimum (the one located at the most negative potential energy value). On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&lt;br /&gt;
&lt;br /&gt;
[[File:Rts.png|frame|right|thumb|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&lt;br /&gt;
[[File:1cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:2cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&lt;br /&gt;
[[File:3cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:4cp.png|thumb]]&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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&lt;br /&gt;
[[File:5cp.png|thumb]]&lt;br /&gt;
&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in higher energy level (more negative in potential energy values) than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
[[File:exooo.png|thumb|frame|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
The reactants H and HF lie in lower energy level (less negative in potential energy values) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:endoo.png|thumb|frame|Figure 4- energy pathway for an endothermic reaction]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines. For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&lt;br /&gt;
[[File:tshf.png|thumb|frame|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1]]&lt;br /&gt;
For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&lt;br /&gt;
[[File:hh.png|thumb|frame|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2]]&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806025</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806025"/>
		<updated>2020-05-16T09:29:38Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 1: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold) linking reactants and reactants is plotted, the transition state is the minimum (the one located at the most negative potential energy value). On the potential energy surface diagram, it is a saddle point. &lt;br /&gt;
[[File:path1.jpg|200px|right|Figure 1-The minimised energy pathway]]&lt;br /&gt;
Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero.&lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&amp;lt;gallery&amp;gt;&lt;br /&gt;
File: Rts.png|Figure 2-The internuclear distances vs time graph&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&amp;lt;gallery&amp;gt;&lt;br /&gt;
[[File:Rts.png|200px|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:1cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:2cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:3cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:4cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:5cp.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in higher energy level (more negative in potential energy values) than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &amp;lt;gallery&amp;gt;&lt;br /&gt;
File:exooo.png|Figure 3- energy pathway for an exothermic reaction&lt;br /&gt;
&amp;lt;/gallery&amp;gt;The reactants H and HF lie in lower energy level (less negative in potential energy values) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&amp;lt;gallery&amp;gt;&lt;br /&gt;
[[File:exooo.png|thumb|right|200px|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:endoo.png|Figure 4- energy pathway for an endothermic reaction&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines. For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:tshf.png|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1&lt;br /&gt;
&amp;lt;/gallery&amp;gt;For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:hh.png|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2&lt;br /&gt;
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== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold) linking reactants and reactants is plotted, the transition state is the minimum (the one located at the most negative potential energy value). On the potential energy surface diagram, it is a saddle point. &amp;lt;gallery&amp;gt;&lt;br /&gt;
File:path1.jpg|Figure 1-The minimised energy pathway&lt;br /&gt;
&amp;lt;/gallery&amp;gt;Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero. &lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&amp;lt;gallery&amp;gt;&lt;br /&gt;
File: Rts.png|Figure 2-The internuclear distances vs time graph&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&amp;lt;gallery&amp;gt;&lt;br /&gt;
[[File:Rts.png|200px|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:1cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:2cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:3cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:4cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:5cp.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 2: F - H - H system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in higher energy level (more negative in potential energy values) than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &amp;lt;gallery&amp;gt;&lt;br /&gt;
File:exooo.png|Figure 3- energy pathway for an exothermic reaction&lt;br /&gt;
&amp;lt;/gallery&amp;gt;The reactants H and HF lie in lower energy level (less negative in potential energy values) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&amp;lt;gallery&amp;gt;&lt;br /&gt;
[[File:exooo.png|thumb|right|200px|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:endoo.png|Figure 4- energy pathway for an endothermic reaction&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
Different combinations of numbers were tried for distances until there is only one spot on the contour spot and the graph of &amp;quot;internuclear distance vs time&amp;quot; shows straight horizontal lines. For the reaction 1--H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;+F, the position of transition state is at r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm.&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:tshf.png|Figure 5- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 1&lt;br /&gt;
&amp;lt;/gallery&amp;gt;For reaction 2--HF+H, the position of transition state is at the same position, where r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;=74.4 pm and r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;=182 pm. This is because both the two reactions involve interactions between H-H and H-F, with only the differences in bond breaking/forming.&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:hh.png|Figure 6- &amp;quot;Internuclear distance vs time&amp;quot; graph for reaction 2&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
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		<summary type="html">&lt;p&gt;Jy8418: /* Answer 6: */&lt;/p&gt;
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== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold) linking reactants and reactants is plotted, the transition state is the minimum (the one located at the most negative potential energy value). On the potential energy surface diagram, it is a saddle point. &amp;lt;gallery&amp;gt;&lt;br /&gt;
File:path1.jpg|Figure 1-The minimised energy pathway&lt;br /&gt;
&amp;lt;/gallery&amp;gt;Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero. &lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&amp;lt;gallery&amp;gt;&lt;br /&gt;
File: Rts.png|Figure 2-The internuclear distances vs time graph&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&amp;lt;gallery&amp;gt;&lt;br /&gt;
[[File:Rts.png|200px|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:1cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:2cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:3cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:4cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:5cp.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== EXERCISE 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in higher energy level (more negative in potential energy values) than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &amp;lt;gallery&amp;gt;&lt;br /&gt;
File:exooo.png|Figure 3- energy pathway for an exothermic reaction&lt;br /&gt;
&amp;lt;/gallery&amp;gt;The reactants H and HF lie in lower energy level (less negative in potential energy values) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&amp;lt;gallery&amp;gt;&lt;br /&gt;
[[File:exooo.png|thumb|right|200px|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:endoo.png|Figure 4- energy pathway for an endothermic reaction&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806008</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=806008"/>
		<updated>2020-05-16T08:48:17Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 5: */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold) linking reactants and reactants is plotted, the transition state is the minimum (the one located at the most negative potential energy value). On the potential energy surface diagram, it is a saddle point. &amp;lt;gallery&amp;gt;&lt;br /&gt;
File:path1.jpg|Figure 1-The minimised energy pathway&lt;br /&gt;
&amp;lt;/gallery&amp;gt;Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero. &lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&amp;lt;gallery&amp;gt;&lt;br /&gt;
File: Rts.png|Figure 2-The internuclear distances vs time graph&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&amp;lt;gallery&amp;gt;&lt;br /&gt;
[[File:Rts.png|200px|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:1cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:2cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:3cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:4cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:5cp.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;br /&gt;
The transition state theory (TST) predicts a higher rate value than the actual experimental value gives. TST assumes that all the trajectories with the energy path along the reaction coordinates greater than the activation energy will be reactive, by ignoring the fact that atoms may &#039;bounce&#039; around the transition state region. By looking at example 4 in the above table, atoms have enough energy but the reaction failed. In this case, TST failed. Also, even though the reaction can proceed under sufficient energy, the time taken for &#039;bouncing around&#039; also reduce the actual rate constant (e.g. example 5), making TST overestimate the rate constant. &lt;br /&gt;
&lt;br /&gt;
== EXERCISE 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
==== Question 6 (PES inspection): ====&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;
==== Answer 6: ====&lt;br /&gt;
The reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and the reaction between H and HF is endothermic. &lt;br /&gt;
&lt;br /&gt;
On the surface plot, the reactants H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and F lie in higher energy level (more negative in potential energy values) than the products, so the reaction is exothermic. (Figure 3, with reactants on RHS and products on LHS). &lt;br /&gt;
&lt;br /&gt;
The reactants H and HF lie in lower energy level (less negative in potential energy values) than the products, so it&#039;s endothermic. (Figure 4, with reactants on LHS and products on RHS)&amp;lt;gallery&amp;gt;&lt;br /&gt;
[[File:exooo.png|thumb|right|200px|Figure 3- energy pathway for an exothermic reaction]]&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:endoo.png|Figure 4- energy pathway for an endothermic reaction&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Bond dissociation energy at 298 K (kJ/mol)&lt;br /&gt;
|-&lt;br /&gt;
|H-H&lt;br /&gt;
|436&lt;br /&gt;
|-&lt;br /&gt;
|H-F&lt;br /&gt;
|569&lt;br /&gt;
|}&lt;br /&gt;
For reaction between F and H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, H-F bond is newly formed and H-H is broken. It has a higher bond energy than H-H does, indicating more energy released, so the reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
The reverse process takes place for reaction between HF and H, H-F is broken and H-H is formed. Therefore, more energy is absorbed to break the strong H-bond H-F and less energy released, so it is an endothermic reaction.&lt;br /&gt;
&lt;br /&gt;
==== Question 7 (PES inspection): ====&lt;br /&gt;
Locate the approximate position of the transition state.&lt;br /&gt;
&lt;br /&gt;
==== Answer 7: ====&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt;https://aip.scitation.org/doi/pdf/10.1063/1.1672005&amp;lt;/nowiki&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:5cp.png&amp;diff=805996</id>
		<title>File:5cp.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:5cp.png&amp;diff=805996"/>
		<updated>2020-05-16T04:33:52Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: &lt;/p&gt;
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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:4cp.png&amp;diff=805995</id>
		<title>File:4cp.png</title>
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		<updated>2020-05-16T04:33:21Z</updated>

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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=805994</id>
		<title>01485762jy</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01485762jy&amp;diff=805994"/>
		<updated>2020-05-16T04:32:21Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: /* Answer 4: */&lt;/p&gt;
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== &#039;&#039;&#039;EXERCISE 1: H + H2 system&#039;&#039;&#039; ==&lt;br /&gt;
&lt;br /&gt;
==== Question 1 (Dynamics from the transition state region): ====&lt;br /&gt;
On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?&lt;br /&gt;
&lt;br /&gt;
==== Answer 1: ====&lt;br /&gt;
On a potential energy surface diagram, the transition state is defined mathematically as following:&lt;br /&gt;
δV/δr&amp;lt;sub&amp;gt;1 &amp;lt;/sub&amp;gt;=&amp;lt;sub&amp;gt; &amp;lt;/sub&amp;gt;δV/δr&amp;lt;sub&amp;gt;2 &amp;lt;/sub&amp;gt;= 0, where V is the chemical potential, r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are the distances between atoms A &amp;amp; B and atoms B &amp;amp; C respectively. &lt;br /&gt;
&lt;br /&gt;
On a reaction co-ordinate diagram, where the minimum energy path (the line in bold) linking reactants and reactants is plotted, the transition state is the minimum (the one located at the most negative potential energy value). On the potential energy surface diagram, it is a saddle point. &amp;lt;gallery&amp;gt;&lt;br /&gt;
File:path1.jpg|Figure 1-The minimised energy pathway&lt;br /&gt;
&amp;lt;/gallery&amp;gt;Both the saddle point and the local minimum have the first derivative equal to zero, but they are distinguished by the following method. For the collision between three homogeneous atoms, the transition state is when r&amp;lt;sub&amp;gt;AB &amp;lt;/sub&amp;gt;= r&amp;lt;sub&amp;gt;BC. &amp;lt;/sub&amp;gt;Other turning points are classified as local maximum/minimum (depends on how you &#039;rotate&#039; the diagram). Mathematically, for collisions between heterogeneous atoms, the term f&amp;lt;sub&amp;gt;xx​(x0​,y0​)&amp;lt;/sub&amp;gt;*&amp;lt;sub&amp;gt;fyy​(x0​,y0​)&amp;lt;/sub&amp;gt;−f&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;xy​(x0​,y0​)&amp;lt;/sub&amp;gt; has to be calculated, where fxx is the second derivative with respect to x, fyy to y and fxy is to differentiate with respect to x then to y. If the term is less than zero, then the coordinate a saddle point. If the term is greater than zero, then the coordinate is a minimum/maximum. For a local minimum, Its second derivative (fxx or fyy) has to be greater than zero. &lt;br /&gt;
&lt;br /&gt;
==== Question 2 (Trajectories from r1 = r2: locating the transition state): ====&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;
&lt;br /&gt;
==== Answer 2: ====&lt;br /&gt;
The best estimate of the transition state position (rts) is r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt;=90.8 pm.  The possible range of transition state is between 85 pm to 110 pm from the surface plot, so the values were tested in this range, keeping r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;BC &amp;lt;/sub&amp;gt;and momentum zero. This result was verified by plotting the “Internuclear Distances vs Time” graph. Two straight horizontal lines at the same height were obtained, indicating the constant distances between A &amp;amp; B and B &amp;amp; C. There is no oscillations on the ridge.&amp;lt;gallery&amp;gt;&lt;br /&gt;
File: Rts.png|Figure 2-The internuclear distances vs time graph&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&amp;lt;gallery&amp;gt;&lt;br /&gt;
[[File:Rts.png|200px|Figure 2-The &amp;quot;Internuclear distances vs Time&amp;quot; graph]]&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Question 3 (Calculating the reaction path): ====&lt;br /&gt;
Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&lt;br /&gt;
&lt;br /&gt;
==== Answer 3: ====&lt;br /&gt;
From the “Internuclear Distances vs Time” graphs generated by two methods, it is found that the distance between atoms A and B is higher in the Dynamics method and tend to infinity, whereas the distance generated by MEP tends to converge at a lower value. Therefore, it can be deduced that MEP is based on the conservation of energy whereas Dynamics ignores that. Also, there are some oscillations in distance B-C when using Dynamics, whereas MEP does not. So MEP ignores the motion of atoms and their inertia.&lt;br /&gt;
&lt;br /&gt;
==== Question 4 (Reactive and unreactive trajectories): ====&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. What can you conclude from the table?&lt;br /&gt;
&lt;br /&gt;
==== Answer 4: ====&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;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;C &amp;lt;/sub&amp;gt;atom and the kinetic barrier is overcome, forming a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The newly formed molecule vibrates away and H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;also moves back.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:1cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-420.077&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves towards H&amp;lt;sub&amp;gt;c &amp;lt;/sub&amp;gt;atom, but the energy was too low to pass the transition state region, so no reaction takes place; the H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; vibrate backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:2cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-413.977&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The vibrating H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) approaches H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; atom and form a new H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;). The new molecule vibrates away.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:3cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-359.277&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Unreactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; reforms bonds with H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and the molecule vibrates backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:4cp.png|&lt;br /&gt;
&amp;lt;/gallery&amp;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;
|&amp;lt;nowiki&amp;gt;-349.477&amp;lt;/nowiki&amp;gt;&lt;br /&gt;
|Reactive&lt;br /&gt;
|The H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule(H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;) moves fast towards H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. The transition state region was crossed. Due to the high momentum, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bounces between H&amp;lt;sub&amp;gt;A &amp;lt;/sub&amp;gt;and H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;. Finally, H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forms new bonds with H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; and the new molecule(H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;) vibrates backwards.&lt;br /&gt;
|&amp;lt;gallery&amp;gt;&lt;br /&gt;
File:5cp.png&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
In conclusion, the momentum of the reactants is crucial in determining the success of reactions. If the momentum is too small, the energy barrier cannot be overcome and the trajectory is unreactive. If the momentum is too large, the transition state region can certainly be crossed, but the atoms may bounce around and the outcome is unpredictable, products are likely to be formed when one momentum is more than double of the other. From the above experimental data, the &#039;safest&#039; p1 is around -3.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;and p2 is -5.1 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==== Question 5 (Transition State Theory): ====&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;
==== Answer 5: ====&lt;/div&gt;</summary>
		<author><name>Jy8418</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:3cp.png&amp;diff=805993</id>
		<title>File:3cp.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:3cp.png&amp;diff=805993"/>
		<updated>2020-05-16T04:06:22Z</updated>

		<summary type="html">&lt;p&gt;Jy8418: &lt;/p&gt;
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