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		<updated>2019-05-24T16:59:19Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Molecular Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate states how the transition state (TS) of a given reaction will resemble either the reactants or the products depending which one is closer in energy. i.e. For an endothermic reaction, the products are closer in energy, and therefore in structure to the transition state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039;  The TS will resemble the reactants in structure as they are closer in energy than the products, and therefore the TS will be located at a position where the distance between the reactants i.e. H-H (BC), is smaller than that of the products i.e. H-F (AB). In other words,  BC&amp;lt;AB depicted by the bottom graph showing the inter-nuclear distance vs time.&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.812 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; The TS will resemble the products in structure as they are closer in energy to it than the reactants, and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC), is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 Å&lt;br /&gt;
&lt;br /&gt;
H-H (AB) bond distance= 0.745 Å&lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Reactants = -103.901 kcal. mol-1 &lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--103.901 = 0.149 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants was calculated using a MEP type calculation by adding 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.912 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the reactants (BC) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Ezo_con.png|frameless|500px|center]]&lt;br /&gt;
[[File:Exoo.png ‎|frameless|500px|center]]&lt;br /&gt;
[[File:Exothermic recation ea.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graphs shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the reactant&#039;s energy (BC) and demonstrates how the activation energy for the F + H-H reaction is approximately 0.149 kcal. mol-1.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Products = -133.965 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--133.965 = 30.213 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the products was calculated using a MEP type calculation by subtracting 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.712 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the products (AB) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Enoconn.png|frameless|500px|center]]&lt;br /&gt;
[[File:Endoevstime.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graph shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the product&#039;s energy (AB) and demonstrates how the activation energy for the H + H-F reaction is approximately 30.213 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
The initial set of conditions that yield a reactive trajectory for the &#039;&#039;&#039; F + H-H → H-F + H&#039;&#039;&#039; are the following:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.74 Å &lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 2 Å &lt;br /&gt;
&lt;br /&gt;
p&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;= -2.001 kg. ms-1&lt;br /&gt;
&lt;br /&gt;
p&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;= -0.501 kg. ms-1&lt;br /&gt;
&lt;br /&gt;
The following graph demonstrates the reactive trajectory:&lt;br /&gt;
&lt;br /&gt;
[[File:Reactuvetraj.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
A plot of Energy vs Time under the reaction conditions described above demonstrates how the total energy of the system is conserved as it remains constant, depicted by a straight green line in the following graph:&lt;br /&gt;
&lt;br /&gt;
[[File:Conservation_ofenergyexo.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Any decrease in potential energy is compensated by a corresponding increase in the kinetic energy and vice versa, resulting in an overall constant total energy. In other words, there is no net loss or gain of energy, but instead energy is being converted from one form into another which basically describes the law of conservation of energy.&lt;br /&gt;
In this example, as the reactant molecules for instance gain kinetic energy, which results in them moving faster, they lose the equivalent amount of potential energy. This could be confirmed experimentally through calorimetry measurements.&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793562</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793562"/>
		<updated>2019-05-24T16:57:20Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Molecular Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate states how the transition state (TS) of a given reaction will resemble either the reactants or the products depending which one is closer in energy. i.e. For an endothermic reaction, the products are closer in energy, and therefore in structure to the transition state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039;  The TS will resemble the reactants in structure as they are closer in energy than the products, and therefore the TS will be located at a position where the distance between the reactants i.e. H-H (BC), is smaller than that of the products i.e. H-F (AB). In other words,  BC&amp;lt;AB depicted by the bottom graph showing the inter-nuclear distance vs time.&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.812 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; The TS will resemble the products in structure as they are closer in energy to it than the reactants, and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC), is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 Å&lt;br /&gt;
&lt;br /&gt;
H-H (AB) bond distance= 0.745 Å&lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Reactants = -103.901 kcal. mol-1 &lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--103.901 = 0.149 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants was calculated using a MEP type calculation by adding 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.912 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the reactants (BC) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Ezo_con.png|frameless|500px|center]]&lt;br /&gt;
[[File:Exoo.png ‎|frameless|500px|center]]&lt;br /&gt;
[[File:Exothermic recation ea.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graphs shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the reactant&#039;s energy (BC) and demonstrates how the activation energy for the F + H-H reaction is approximately 0.149 kcal. mol-1.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Products = -133.965 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--133.965 = 30.213 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the products was calculated using a MEP type calculation by subtracting 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.712 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the products (AB) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Enoconn.png|frameless|500px|center]]&lt;br /&gt;
[[File:Endoevstime.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graph shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the product&#039;s energy (AB) and demonstrates how the activation energy for the H + H-F reaction is approximately 30.213 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
The initial set of conditions that yield a reactive trajectory for the &#039;&#039;&#039; F + H-H → H-F + H&#039;&#039;&#039; are the following:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.74 Å &lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 2 Å &lt;br /&gt;
&lt;br /&gt;
p&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;= -2.001 kg. ms-1&lt;br /&gt;
&lt;br /&gt;
p&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;= -0.501 kg. ms-1&lt;br /&gt;
&lt;br /&gt;
The following graph demonstrates the reactive trajectory:&lt;br /&gt;
&lt;br /&gt;
[[File:Reactuvetraj.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
A plot of Energy vs Time under the reaction conditions described above demonstrates how the total energy of the system is conserved as it remains constant, depicted by a straight green line in the following graph:&lt;br /&gt;
&lt;br /&gt;
[[File:Conservation_ofenergyexo.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Any decrease in potential energy is compensated by a corresponding increase in the kinetic energy and vice versa, resulting in an overall constant total energy. In other words, there is no net loss or gain of energy, but instead energy is being converted from one form into another which basically describes the law of conservation of energy.&lt;br /&gt;
In this example, as the reactant molecules for instance gain kinetic energy, which results in them moving faster, they lose the equivalent amount of potential energy.&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793542</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793542"/>
		<updated>2019-05-24T16:48:34Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Molecular Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate states how the transition state (TS) of a given reaction will resemble either the reactants or the products depending which one is closer in energy. i.e. For an endothermic reaction, the products are closer in energy, and therefore in structure to the transition state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039;  The TS will resemble the reactants in structure as they are closer in energy than the products, and therefore the TS will be located at a position where the distance between the reactants i.e. H-H (BC), is smaller than that of the products i.e. H-F (AB). In other words,  BC&amp;lt;AB depicted by the bottom graph showing the inter-nuclear distance vs time.&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.812 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; The TS will resemble the products in structure as they are closer in energy to it than the reactants, and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC), is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 Å&lt;br /&gt;
&lt;br /&gt;
H-H (AB) bond distance= 0.745 Å&lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Reactants = -103.901 kcal. mol-1 &lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--103.901 = 0.149 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants was calculated using a MEP type calculation by adding 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.912 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the reactants (BC) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Ezo_con.png|frameless|500px|center]]&lt;br /&gt;
[[File:Exoo.png ‎|frameless|500px|center]]&lt;br /&gt;
[[File:Exothermic recation ea.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graphs shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the reactant&#039;s energy (BC) and demonstrates how the activation energy for the F + H-H reaction is approximately 0.149 kcal. mol-1.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Products = -133.965 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--133.965 = 30.213 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the products was calculated using a MEP type calculation by subtracting 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.712 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the products (AB) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Enoconn.png|frameless|500px|center]]&lt;br /&gt;
[[File:Endoevstime.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graph shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the product&#039;s energy (AB) and demonstrates how the activation energy for the H + H-F reaction is approximately 30.213 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
The initial set of conditions that yield a reactive trajectory for the &#039;&#039;&#039; F + H-H → H-F + H&#039;&#039;&#039; are the following:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.74 Å &lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 2 Å &lt;br /&gt;
&lt;br /&gt;
p&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;= -2.001 kg. ms-1&lt;br /&gt;
&lt;br /&gt;
p&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;= -0.501 kg. ms-1&lt;br /&gt;
&lt;br /&gt;
The following graph demonstrates the reactive trajectory:&lt;br /&gt;
&lt;br /&gt;
[[File:Reactuvetraj.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
A plot of Energy vs Time under the reaction conditions described above demonstrates how the total energy of the system is conserved as it remains constant, depicted by a straight green line in the following graph:&lt;br /&gt;
&lt;br /&gt;
[[File:Conservation_ofenergyexo.png ‎|frameless|500px|center]]&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Conservation_ofenergyexo.png&amp;diff=793538</id>
		<title>File:Conservation ofenergyexo.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Conservation_ofenergyexo.png&amp;diff=793538"/>
		<updated>2019-05-24T16:48:05Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793504</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793504"/>
		<updated>2019-05-24T16:42:08Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Molecular Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate states how the transition state (TS) of a given reaction will resemble either the reactants or the products depending which one is closer in energy. i.e. For an endothermic reaction, the products are closer in energy, and therefore in structure to the transition state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039;  The TS will resemble the reactants in structure as they are closer in energy than the products, and therefore the TS will be located at a position where the distance between the reactants i.e. H-H (BC), is smaller than that of the products i.e. H-F (AB). In other words,  BC&amp;lt;AB depicted by the bottom graph showing the inter-nuclear distance vs time.&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.812 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; The TS will resemble the products in structure as they are closer in energy to it than the reactants, and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC), is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 Å&lt;br /&gt;
&lt;br /&gt;
H-H (AB) bond distance= 0.745 Å&lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Reactants = -103.901 kcal. mol-1 &lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--103.901 = 0.149 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants was calculated using a MEP type calculation by adding 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.912 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the reactants (BC) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Ezo_con.png|frameless|500px|center]]&lt;br /&gt;
[[File:Exoo.png ‎|frameless|500px|center]]&lt;br /&gt;
[[File:Exothermic recation ea.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graphs shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the reactant&#039;s energy (BC) and demonstrates how the activation energy for the F + H-H reaction is approximately 0.149 kcal. mol-1.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Products = -133.965 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--133.965 = 30.213 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the products was calculated using a MEP type calculation by subtracting 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.712 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the products (AB) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Enoconn.png|frameless|500px|center]]&lt;br /&gt;
[[File:Endoevstime.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graph shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the product&#039;s energy (AB) and demonstrates how the activation energy for the H + H-F reaction is approximately 30.213 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
The initial set of conditions that yield a reactive trajectory for the &#039;&#039;&#039; F + H-H → H-F + H&#039;&#039;&#039; are the following:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.74 Å &lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 2 Å &lt;br /&gt;
&lt;br /&gt;
p&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt;= -2.001 kg. ms-1&lt;br /&gt;
&lt;br /&gt;
p&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt;= -0.501 kg. ms-1&lt;br /&gt;
&lt;br /&gt;
The following graph demonstrates the reactive trajectory:&lt;br /&gt;
&lt;br /&gt;
[[File:Reactuvetraj.png ‎|frameless|500px|center]]&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Reactuvetraj.png&amp;diff=793503</id>
		<title>File:Reactuvetraj.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Reactuvetraj.png&amp;diff=793503"/>
		<updated>2019-05-24T16:41:54Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793463</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793463"/>
		<updated>2019-05-24T16:29:42Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Reaction dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate states how the transition state (TS) of a given reaction will resemble either the reactants or the products depending which one is closer in energy. i.e. For an endothermic reaction, the products are closer in energy, and therefore in structure to the transition state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039;  The TS will resemble the reactants in structure as they are closer in energy than the products, and therefore the TS will be located at a position where the distance between the reactants i.e. H-H (BC), is smaller than that of the products i.e. H-F (AB). In other words,  BC&amp;lt;AB depicted by the bottom graph showing the inter-nuclear distance vs time.&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.812 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; The TS will resemble the products in structure as they are closer in energy to it than the reactants, and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC), is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 Å&lt;br /&gt;
&lt;br /&gt;
H-H (AB) bond distance= 0.745 Å&lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Reactants = -103.901 kcal. mol-1 &lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--103.901 = 0.149 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants was calculated using a MEP type calculation by adding 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.912 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the reactants (BC) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Ezo_con.png|frameless|500px|center]]&lt;br /&gt;
[[File:Exoo.png ‎|frameless|500px|center]]&lt;br /&gt;
[[File:Exothermic recation ea.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graphs shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the reactant&#039;s energy (BC) and demonstrates how the activation energy for the F + H-H reaction is approximately 0.149 kcal. mol-1.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Products = -133.965 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--133.965 = 30.213 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the products was calculated using a MEP type calculation by subtracting 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.712 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the products (AB) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Enoconn.png|frameless|500px|center]]&lt;br /&gt;
[[File:Endoevstime.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graph shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the product&#039;s energy (AB) and demonstrates how the activation energy for the H + H-F reaction is approximately 30.213 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
The initial set of conditions that yield a reactive trajectory for the &#039;&#039;&#039; F + H-H → H-F + H&#039;&#039;&#039; are the following:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793445</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793445"/>
		<updated>2019-05-24T16:26:49Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Report the activation energy for both reactions. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate states how the transition state (TS) of a given reaction will resemble either the reactants or the products depending which one is closer in energy. i.e. For an endothermic reaction, the products are closer in energy, and therefore in structure to the transition state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039;  The TS will resemble the reactants in structure as they are closer in energy than the products, and therefore the TS will be located at a position where the distance between the reactants i.e. H-H (BC), is smaller than that of the products i.e. H-F (AB). In other words,  BC&amp;lt;AB depicted by the bottom graph showing the inter-nuclear distance vs time.&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.812 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; The TS will resemble the products in structure as they are closer in energy to it than the reactants, and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC), is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 Å&lt;br /&gt;
&lt;br /&gt;
H-H (AB) bond distance= 0.745 Å&lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Reactants = -103.901 kcal. mol-1 &lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--103.901 = 0.149 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants was calculated using a MEP type calculation by adding 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.912 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the reactants (BC) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Ezo_con.png|frameless|500px|center]]&lt;br /&gt;
[[File:Exoo.png ‎|frameless|500px|center]]&lt;br /&gt;
[[File:Exothermic recation ea.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graphs shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the reactant&#039;s energy (BC) and demonstrates how the activation energy for the F + H-H reaction is approximately 0.149 kcal. mol-1.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Products = -133.965 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--133.965 = 30.213 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the products was calculated using a MEP type calculation by subtracting 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.712 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the products (AB) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Enoconn.png|frameless|500px|center]]&lt;br /&gt;
[[File:Endoevstime.png ‎|frameless|500px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graph shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the product&#039;s energy (AB) and demonstrates how the activation energy for the H + H-F reaction is approximately 30.213 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793440</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793440"/>
		<updated>2019-05-24T16:25:22Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Report the activation energy for both reactions. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate states how the transition state (TS) of a given reaction will resemble either the reactants or the products depending which one is closer in energy. i.e. For an endothermic reaction, the products are closer in energy, and therefore in structure to the transition state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039;  The TS will resemble the reactants in structure as they are closer in energy than the products, and therefore the TS will be located at a position where the distance between the reactants i.e. H-H (BC), is smaller than that of the products i.e. H-F (AB). In other words,  BC&amp;lt;AB depicted by the bottom graph showing the inter-nuclear distance vs time.&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.812 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; The TS will resemble the products in structure as they are closer in energy to it than the reactants, and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC), is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 Å&lt;br /&gt;
&lt;br /&gt;
H-H (AB) bond distance= 0.745 Å&lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Reactants = -103.901 kcal. mol-1 &lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--103.901 = 0.149 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants was calculated using a MEP type calculation by adding 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.912 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the reactants (BC) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Ezo_con.png|frameless|350px|center]]&lt;br /&gt;
[[File:Exoo.png ‎|frameless|350px|center]]&lt;br /&gt;
[[File:Exothermic recation ea.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graphs shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the reactant&#039;s energy (BC) and demonstrates how the activation energy for the F + H-H reaction is approximately 0.149 kcal. mol-1.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Products = -133.965 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--133.965 = 30.213 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the products was calculated using a MEP type calculation by subtracting 0.1 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.712 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the products (AB) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Enoconn.png|frameless|350px|center]]&lt;br /&gt;
[[File:Endoevstime.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graph shows the step in energy (E&amp;lt;sub&amp;gt;a&amp;lt;/sub&amp;gt;) between the the transition state energy and the product&#039;s energy (AB) and demonstrates how the activation energy for the H + H-F reaction is approximately 30.213 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Exothermic_recation_ea.png&amp;diff=793437</id>
		<title>File:Exothermic recation ea.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Exothermic_recation_ea.png&amp;diff=793437"/>
		<updated>2019-05-24T16:25:03Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Exoo.png&amp;diff=793431</id>
		<title>File:Exoo.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Exoo.png&amp;diff=793431"/>
		<updated>2019-05-24T16:24:09Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Ezo_con.png&amp;diff=793417</id>
		<title>File:Ezo con.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Ezo_con.png&amp;diff=793417"/>
		<updated>2019-05-24T16:21:57Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Enoconn.png&amp;diff=793413</id>
		<title>File:Enoconn.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Enoconn.png&amp;diff=793413"/>
		<updated>2019-05-24T16:21:21Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Endoevstime.png&amp;diff=793408</id>
		<title>File:Endoevstime.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Endoevstime.png&amp;diff=793408"/>
		<updated>2019-05-24T16:20:49Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793158</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793158"/>
		<updated>2019-05-24T15:36:15Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Report the activation energy for both reactions. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate states how the transition state (TS) of a given reaction will resemble either the reactants or the products depending which one is closer in energy. i.e. For an endothermic reaction, the products are closer in energy, and therefore in structure to the transition state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039;  The TS will resemble the reactants in structure as they are closer in energy than the products, and therefore the TS will be located at a position where the distance between the reactants i.e. H-H (BC), is smaller than that of the products i.e. H-F (AB). In other words,  BC&amp;lt;AB depicted by the bottom graph showing the inter-nuclear distance vs time.&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.812 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; The TS will resemble the products in structure as they are closer in energy to it than the reactants, and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC), is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 Å&lt;br /&gt;
&lt;br /&gt;
H-H (AB) bond distance= 0.745 Å&lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--103.866 = 0.114 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants was calculated using a MEP type calculation by subtracting 0.2 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
1.81&lt;br /&gt;
H-F (AB) bond distance= 1.612 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the products (AB distance decreases) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Energytime_exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graph shows the step in energy between the the reactants and the transition state (i.e. the activation energy).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Reactants = -133.453 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793103</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793103"/>
		<updated>2019-05-24T15:23:43Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Report the activation energy for both reactions. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate states how the transition state (TS) of a given reaction will resemble either the reactants or the products depending which one is closer in energy. i.e. For an endothermic reaction, the products are closer in energy, and therefore in structure to the transition state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039;  The TS will resemble the reactants in structure as they are closer in energy than the products, and therefore the TS will be located at a position where the distance between the reactants i.e. H-H (BC), is smaller than that of the products i.e. H-F (AB). In other words,  BC&amp;lt;AB depicted by the bottom graph showing the inter-nuclear distance vs time.&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.812 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; The TS will resemble the products in structure as they are closer in energy to it than the reactants, and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC), is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 Å&lt;br /&gt;
&lt;br /&gt;
H-H (AB) bond distance= 0.745 Å&lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--103.866 = 0.114 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants was calculated using a MEP type calculation by subtracting 0.2 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.612 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the products (AB distance decreases) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Energytime_exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The bottom graph shows the step in energy between the the reactants and the transition state (i.e. the activation energy).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Energytime_exo.png&amp;diff=793084</id>
		<title>File:Energytime exo.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Energytime_exo.png&amp;diff=793084"/>
		<updated>2019-05-24T15:20:47Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793074</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=793074"/>
		<updated>2019-05-24T15:18:17Z</updated>

		<summary type="html">&lt;p&gt;El917: /* EXERCISE 2: F-H-H system */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; (2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate states how the transition state (TS) of a given reaction will resemble either the reactants or the products depending which one is closer in energy. i.e. For an endothermic reaction, the products are closer in energy, and therefore in structure to the transition state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039;  The TS will resemble the reactants in structure as they are closer in energy than the products, and therefore the TS will be located at a position where the distance between the reactants i.e. H-H (BC), is smaller than that of the products i.e. H-F (AB). In other words,  BC&amp;lt;AB depicted by the bottom graph showing the inter-nuclear distance vs time.&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.812 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; The TS will resemble the products in structure as they are closer in energy to it than the reactants, and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC), is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 Å&lt;br /&gt;
&lt;br /&gt;
H-H (AB) bond distance= 0.745 Å&lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039; &lt;br /&gt;
&lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
&lt;br /&gt;
So the &#039;&#039;&#039;activation energy= -103.752--103.866 = 0.114 kcal. mol-1&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The energy of the reactants was calculated using a MEP type calculation by subtracting 0.2 Å to the H-F (AB) bond length while the rest of the conditions were kept constant yielding the following conditions: &lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.612 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
As a result, the reaction trajectory was pushed towards the products (AB distance decreases) and the MEP calculations yielded the following graphs:&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792914</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792914"/>
		<updated>2019-05-24T14:51:02Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Locate the approximate position of the transition state. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; 1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; 2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate states how the transition state (TS) of a given reaction will resemble either the reactants or the products depending which one is closer in energy. i.e. For an endothermic reaction, the products are closer in energy, and therefore in structure to the transition state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039;  The TS will resemble the reactants in structure as they are closer in energy than the products, and therefore the TS will be located at a position where the distance between the reactants i.e. H-H (BC), is smaller than that of the products i.e. H-F (AB). In other words,  BC&amp;lt;AB depicted by the bottom graph showing the inter-nuclear distance vs time.&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.812 Å &lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(2) Endothermic Reaction:&#039;&#039;&#039; The TS will resemble the products in structure as they are closer in energy to it than the reactants, and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC), is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 Å&lt;br /&gt;
&lt;br /&gt;
H-H (AB) bond distance= 0.745 Å&lt;br /&gt;
&lt;br /&gt;
(p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792887</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792887"/>
		<updated>2019-05-24T14:47:29Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Locate the approximate position of the transition state. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; 1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; 2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate states how the transition state (TS) of a given reaction will resemble either the reactants or the products depending which one is closer in energy. i.e. For an endothermic reaction, the products are closer in energy, and therefore in structure to the transition state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;(1) Exothermic Reaction:&#039;&#039;&#039;  The TS will resemble the reactants in structure as they are closer in energy than the products, and therefore the TS will be located at a position where the distance between the reactants i.e. H-H (BC), is smaller than that of the products i.e. H-F (AB). In other words,  BC&amp;lt;AB depicted by the bottom graph showing the inter-nuclear distance vs time.&lt;br /&gt;
&lt;br /&gt;
So at the TS:&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 Å and&lt;br /&gt;
&lt;br /&gt;
H-F (AB) bond distance= 1.812 Å &lt;br /&gt;
&lt;br /&gt;
(p1=p2=0)&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792828</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792828"/>
		<updated>2019-05-24T14:36:23Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; 1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.74 Å; H-F (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=F, B=H and C=H respectively.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; 2) H + H-F → H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) bond distance= 0.91 Å; H-H (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) bond distance= 2.3 Å; p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 kg ms-1; p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where atom A=H, B=H and C=F respectively. &lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small compared to the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792770</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792770"/>
		<updated>2019-05-24T14:21:21Z</updated>

		<summary type="html">&lt;p&gt;El917: /* PES inspection */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the (1) F + H2 and (2) H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; 1) F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 Å&lt;br /&gt;
H-F (r2) bond distance= 2.3 Å&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 Å&lt;br /&gt;
H-H (r2) bond distance= 2.3 Å&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792769</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792769"/>
		<updated>2019-05-24T14:20:03Z</updated>

		<summary type="html">&lt;p&gt;El917: /* PES inspection */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; → F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 Å&lt;br /&gt;
H-F (r2) bond distance= 2.3 Å&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 Å&lt;br /&gt;
H-H (r2) bond distance= 2.3 Å&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792755</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792755"/>
		<updated>2019-05-24T14:17:04Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
&lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
&lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792752</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792752"/>
		<updated>2019-05-24T14:16:33Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
The main assumptions of the transition state theory are the following:&lt;br /&gt;
&lt;br /&gt;
1) The reactants and the transition state are in equilibrium. &lt;br /&gt;
2) The energy of the reactant particles is described by the Boltzmann distribution. &lt;br /&gt;
3) &#039;&#039;&#039; If reactants reach the transition state, the latter does not collapse back to the reactants and the reaction progresses into the products&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
In this case, the most relevant assumption is the third one, which implies that once the transition state is reached the reaction always progresses into the products but we know this is not true from the experimental data shown in the table above. Reaction 4 above represents a barrier recrossing, which as previously described shows how the system crosses the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, however, this collapses back into the products reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond. The TST would predict this trajectory to be reactive but experimental values show otherwise.&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792600</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792600"/>
		<updated>2019-05-24T13:47:03Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond, however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert back and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792577</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792577"/>
		<updated>2019-05-24T13:43:46Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond unchanged. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as atom H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;; however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Look at animations to comment on the dynamics (trajectory) of the reaction. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792571</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792571"/>
		<updated>2019-05-24T13:42:49Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation energy and the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; left bond unbroken. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as atom H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;; however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Look at animations to comment on the dynamics (trajectory) of the reaction. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792562</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792562"/>
		<updated>2019-05-24T13:41:35Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however, the system does not have the enough energy to overcome the activation barrier and therefore the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub bond unbroken. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as atom H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;; however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Look at animations to comment on the dynamics (trajectory) of the reaction. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792559</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792559"/>
		<updated>2019-05-24T13:41:17Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Reactive and unreactive trajectories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially, however the system does not have the enough energy to overcome the activation barrier and therefore the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub bond unbroken. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as atom H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;; however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Look at animations to comment on the dynamics (trajectory) of the reaction. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792553</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792553"/>
		<updated>2019-05-24T13:39:58Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Molecular Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially as however the system does not have the enough energy to overcome the activation barrier and therefore the system returns to the initial conditions with the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub bond unbroken. The trajectory is non reactive. ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || This reaction resembles the first one as H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and AB distance decreases, the system has sufficient energy to react and overcome the energy barrier leading to the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming. ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| This profile is different to the ones previously described as the system has enough energy to react, and the AB distance decreases as atom H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; approaches the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;; however, once the system passes the transition state and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms, this subsequently breaks again reforming the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond and reverting the reaction back to the reactants.  ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-83.416||Reactive ||This is kind of a special case as well, as the reaction takes place and the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond forms as the system overcomes the energy barrier but this subsequently breaks reforming the reactants. However, in this case the system does not fully revert and the reaction takes place a second time forming the H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; bond and breaking the H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; one.  ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Look at animations to comment on the dynamics (trajectory) of the reaction. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792214</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=792214"/>
		<updated>2019-05-24T13:00:25Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;)/∂r&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Saddle_good.png|frameless|1000px|center]]&lt;br /&gt;
Where A, B and C are the three H atoms respectively; The intersection between the arrows (yellow cross) represents the transitions state.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the top. By contrast, the dynamic plot shows how the trajectory of the reaction oscillates as it takes into account the vibrational energies the atoms possess.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demonstrating how the momentum of the system is constant regardless of the values you input for p1 and p2 in the mep representation (bottom graph). However, the momentum is seen to change with time in a dynamic plot as although it takes the translation energy to = 0 (i.e. p1=p2=0), it accounts for the vibrational quantised energies of the molecules which accounts for the variation in momentum (top graph).&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; → H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; + H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where unchanged throughout with r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; (BC)= 0.74 Å and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; (AB) = 2.0 Å; the red cross on the plots represents the &#039;&#039;&#039;start&#039;&#039;&#039; of the trajectory.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially and eventually the system crosses the transition state with H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;C&amp;lt;/sub&amp;gt; bond breaking and H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt;-H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; forming and hence BC (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;) distance increases. ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || The distance between H&amp;lt;sub&amp;gt;A&amp;lt;/sub&amp;gt; and H&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; (r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) decreases initially ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-84.956||Reactive || ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Look at animations to comment on the dynamics (trajectory) of the reaction. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Saddle_good.png&amp;diff=791807</id>
		<title>File:Saddle good.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Saddle_good.png&amp;diff=791807"/>
		<updated>2019-05-24T09:51:29Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791806</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791806"/>
		<updated>2019-05-24T09:51:09Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Molecular Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====Dynamics from the transition state region====&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
On a potential energy surface diagram the transition state is mathematically defined as a saddle point, this is not the same as a local maxima or minima. It is the maximum on the minimum energy path relating the reactants to products and therefore is the point on the graph where the slopes in orthogonal directions have partial double derivatives of opposite sign.&lt;br /&gt;
&lt;br /&gt;
In other words, ∂V(ri)/∂ri=0 for all three (maxima, minima and saddle point), i.e. the gradient of the potential energy surface = 0 at all three points.&lt;br /&gt;
&lt;br /&gt;
However, if you take the partial derivatives in opposite directions to the point, you can differentiate between the three as a local minima, for instance, will always have a positive second derivative independent from the plane you measure it relative to. By contrast, a saddle point will have a different second derivative depending on which plane you measure it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the orthogonal direction will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Q1_reaciontrajectory_saddlepoint.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A, B and C are the three H atoms respectively; AB (r2) = 2.3 A with p2= -2.7; BC (r1)= 0.74 A and p1= 0&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r1 = r2 (and p1=p2=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r1=r2) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the mep and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
translational energy=0 but not the vibrational&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the left. By contrast, the dynamic plot shows how the trajectory to the product oscillates as it takes into account the vibrational energies.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demostrating how the momentum of the system is constant regardless of the values you input for p1 and p2. However, the moemntum is seen to change with a dynamic plot as although it takes the translation energy = 0 (i.e. p1=p2=0), it accounts for the vibrational energies of the molecules.&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Reactive and unreactive trajectories====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The initial distances where kept constant throughout with r1 (BC)= 0.74 A and r2 (AB) = 2.0 A.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-84.956||Reactive || ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Look at animations to comment on the dynamics (trajectory) of the reaction. &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====PES inspection====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====Reaction dynamics====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791614</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791614"/>
		<updated>2019-05-23T19:36:58Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Molecular Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?====&lt;br /&gt;
&lt;br /&gt;
The transition state is formally defined as the maximum on the minimum energy path relating the reactants to products, mathematically this is defined by a saddle point which is not the same as a local maxima or minima. The transition state (saddle point) is therefore the point on the potential energy graph where the slopes in orthogonal directions are all opposite.  &lt;br /&gt;
&lt;br /&gt;
∂V(ri)/∂ri=0 for all three, i.e. the gradient of the potential = 0 for all three.&lt;br /&gt;
However, if you take partial derivatives you can differentiate between the three as a local minima, for instance, will always have a positive second derivative. By contrast, a saddle point will have a different second derivative depending on which plane you take it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the opposite direction it will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Q1_reaciontrajectory_saddlepoint.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A, B and C are H atoms; AB (r2) = 2.3 and p2= -2.7; BC (r1)= 0.74 and p1= 0&lt;br /&gt;
&lt;br /&gt;
====Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r1 = r2 (and p1=p2=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r1=r2) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
====Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
translational energy=0 but not the vibrational&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the left. By contrast, the dynamic plot shows how the trajectory to the product oscillates as it takes into account the vibrational energies.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demostrating how the momentum of the system is constant regardless of the values you input for p1 and p2. However, the moemntum is seen to change with a dynamic plot as although it takes the translation energy = 0 (i.e. p1=p2=0), it accounts for the vibrational energies of the molecules.&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
&lt;br /&gt;
The initial distances where kept constant throughout with r1 (BC)= 0.74 A and r2 (AB) = 2.0 A.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-84.956||Reactive || ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Look at animations to comment on the dynamics (trajectory) of the reaction. &lt;br /&gt;
&lt;br /&gt;
====State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791611</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791611"/>
		<updated>2019-05-23T19:32:31Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Molecular Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?====&lt;br /&gt;
&lt;br /&gt;
The transition state is formally defined as the maximum on the minimum energy path relating the reactants to products, mathematically this is defined by a saddle point which is not the same as a local maxima or minima. The transition state (saddle point) is therefore the point on the potential energy graph where the slopes in orthogonal directions are all opposite.  &lt;br /&gt;
&lt;br /&gt;
∂V(ri)/∂ri=0 for all three, i.e. the gradient of the potential = 0 for all three.&lt;br /&gt;
However, if you take partial derivatives you can differentiate between the three as a local minima, for instance, will always have a positive second derivative. By contrast, a saddle point will have a different second derivative depending on which plane you take it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the opposite direction it will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Q1_reaciontrajectory_saddlepoint.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A, B and C are H atoms; AB (r2) = 2.3 and p2= -2.7; BC (r1)= 0.74 and p1= 0&lt;br /&gt;
&lt;br /&gt;
====Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r1 = r2 (and p1=p2=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r1=r2) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
====Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
translational energy=0 but not the vibrational&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the left. By contrast, the dynamic plot shows how the trajectory to the product oscillates as it takes into account the vibrational energies.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demostrating how the momentum of the system is constant regardless of the values you input for p1 and p2. However, the moemntum is seen to change with a dynamic plot as although it takes the translation energy = 0 (i.e. p1=p2=0), it accounts for the vibrational energies of the molecules.&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Barrier Recrossing|| ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-84.956||Reactive || ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Look at animations to comment on the dynamics (trajectory) of the reaction. &lt;br /&gt;
&lt;br /&gt;
====State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791606</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791606"/>
		<updated>2019-05-23T19:29:23Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Molecular Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?====&lt;br /&gt;
&lt;br /&gt;
The transition state is formally defined as the maximum on the minimum energy path relating the reactants to products, mathematically this is defined by a saddle point which is not the same as a local maxima or minima. The transition state (saddle point) is therefore the point on the potential energy graph where the slopes in orthogonal directions are all opposite.  &lt;br /&gt;
&lt;br /&gt;
∂V(ri)/∂ri=0 for all three, i.e. the gradient of the potential = 0 for all three.&lt;br /&gt;
However, if you take partial derivatives you can differentiate between the three as a local minima, for instance, will always have a positive second derivative. By contrast, a saddle point will have a different second derivative depending on which plane you take it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the opposite direction it will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Q1_reaciontrajectory_saddlepoint.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A, B and C are H atoms; AB (r2) = 2.3 and p2= -2.7; BC (r1)= 0.74 and p1= 0&lt;br /&gt;
&lt;br /&gt;
====Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r1 = r2 (and p1=p2=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r1=r2) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
====Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
translational energy=0 but not the vibrational&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the left. By contrast, the dynamic plot shows how the trajectory to the product oscillates as it takes into account the vibrational energies.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demostrating how the momentum of the system is constant regardless of the values you input for p1 and p2. However, the moemntum is seen to change with a dynamic plot as although it takes the translation energy = 0 (i.e. p1=p2=0), it accounts for the vibrational energies of the molecules.&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Not Reactive?|| ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-84.956||Reactive || ||[[File:Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791605</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791605"/>
		<updated>2019-05-23T19:28:40Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Molecular Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?====&lt;br /&gt;
&lt;br /&gt;
The transition state is formally defined as the maximum on the minimum energy path relating the reactants to products, mathematically this is defined by a saddle point which is not the same as a local maxima or minima. The transition state (saddle point) is therefore the point on the potential energy graph where the slopes in orthogonal directions are all opposite.  &lt;br /&gt;
&lt;br /&gt;
∂V(ri)/∂ri=0 for all three, i.e. the gradient of the potential = 0 for all three.&lt;br /&gt;
However, if you take partial derivatives you can differentiate between the three as a local minima, for instance, will always have a positive second derivative. By contrast, a saddle point will have a different second derivative depending on which plane you take it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the opposite direction it will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Q1_reaciontrajectory_saddlepoint.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A, B and C are H atoms; AB (r2) = 2.3 and p2= -2.7; BC (r1)= 0.74 and p1= 0&lt;br /&gt;
&lt;br /&gt;
====Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r1 = r2 (and p1=p2=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r1=r2) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
====Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
translational energy=0 but not the vibrational&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the left. By contrast, the dynamic plot shows how the trajectory to the product oscillates as it takes into account the vibrational energies.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demostrating how the momentum of the system is constant regardless of the values you input for p1 and p2. However, the moemntum is seen to change with a dynamic plot as although it takes the translation energy = 0 (i.e. p1=p2=0), it accounts for the vibrational energies of the molecules.&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956|| Not Reactive?|| ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-84.956||Reactive || ||[[Trajectory_5.1_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Trajectory_5.1_table.png&amp;diff=791604</id>
		<title>File:Trajectory 5.1 table.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Trajectory_5.1_table.png&amp;diff=791604"/>
		<updated>2019-05-23T19:28:19Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791583</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791583"/>
		<updated>2019-05-23T19:07:02Z</updated>

		<summary type="html">&lt;p&gt;El917: /* Molecular Reaction Dynamics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?====&lt;br /&gt;
&lt;br /&gt;
The transition state is formally defined as the maximum on the minimum energy path relating the reactants to products, mathematically this is defined by a saddle point which is not the same as a local maxima or minima. The transition state (saddle point) is therefore the point on the potential energy graph where the slopes in orthogonal directions are all opposite.  &lt;br /&gt;
&lt;br /&gt;
∂V(ri)/∂ri=0 for all three, i.e. the gradient of the potential = 0 for all three.&lt;br /&gt;
However, if you take partial derivatives you can differentiate between the three as a local minima, for instance, will always have a positive second derivative. By contrast, a saddle point will have a different second derivative depending on which plane you take it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the opposite direction it will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
[[File:Q1_reaciontrajectory_saddlepoint.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A, B and C are H atoms; AB (r2) = 2.3 and p2= -2.7; BC (r1)= 0.74 and p1= 0&lt;br /&gt;
&lt;br /&gt;
====Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r1 = r2 (and p1=p2=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r1=r2) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
====Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
translational energy=0 but not the vibrational&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the left. By contrast, the dynamic plot shows how the trajectory to the product oscillates as it takes into account the vibrational energies.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demostrating how the momentum of the system is constant regardless of the values you input for p1 and p2. However, the moemntum is seen to change with a dynamic plot as although it takes the translation energy = 0 (i.e. p1=p2=0), it accounts for the vibrational energies of the molecules.&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956||Not Reactive|| ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-84.956||Reactive || ||[[File:Trajectory_5_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;br /&gt;
&lt;br /&gt;
====Report the activation energy for both reactions.====&lt;br /&gt;
&lt;br /&gt;
The activation energy is formally defined as the energy difference between the transition state and the energy of the reactants.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (exo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants = -103.866 kcal. mol-1 &lt;br /&gt;
latter calculated substracting 0.2 amstrong (AB=1.612 A) to the H-F (AB) bond length. This pushes the reaction into the products. &lt;br /&gt;
Step number=500&lt;br /&gt;
size=0.002&lt;br /&gt;
&lt;br /&gt;
[[File:Contour_Eaexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Contour_Ea.exo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
So the activation energy= -103.752+103.866 = 0.114 kcal. mol-1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (endo):&#039;&#039;&#039; &lt;br /&gt;
Energy of the TS = -103.752 kcal. mol-1&lt;br /&gt;
Energy of the Reactants =&lt;br /&gt;
&lt;br /&gt;
====In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. Explain how this could be confirmed experimentally.====&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Q1_reaciontrajectory_saddlepoint.png&amp;diff=791568</id>
		<title>File:Q1 reaciontrajectory saddlepoint.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Q1_reaciontrajectory_saddlepoint.png&amp;diff=791568"/>
		<updated>2019-05-23T18:58:27Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Ea.exo.png&amp;diff=791536</id>
		<title>File:Contour Ea.exo.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Ea.exo.png&amp;diff=791536"/>
		<updated>2019-05-23T18:41:37Z</updated>

		<summary type="html">&lt;p&gt;El917: El917 uploaded a new version of File:Contour Ea.exo.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Eaexo.png&amp;diff=791535</id>
		<title>File:Contour Eaexo.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Eaexo.png&amp;diff=791535"/>
		<updated>2019-05-23T18:39:18Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Ea.exo.png&amp;diff=791525</id>
		<title>File:Contour Ea.exo.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contour_Ea.exo.png&amp;diff=791525"/>
		<updated>2019-05-23T18:34:41Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791415</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791415"/>
		<updated>2019-05-23T17:27:39Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?====&lt;br /&gt;
&lt;br /&gt;
The transition state is formally defined as the maximum on the minimum energy path relating the reactants to products, mathematically this is defined by a saddle point which is not the same as a local maxima or minima. The transition state (saddle point) is therefore the point on the potential energy graph where the slopes in orthogonal directions are all opposite.  &lt;br /&gt;
&lt;br /&gt;
∂V(ri)/∂ri=0 for all three, i.e. the gradient of the potential = 0 for all three.&lt;br /&gt;
However, if you take partial derivatives you can differentiate between the three as a local minima, for instance, will always have a positive second derivative. By contrast, a saddle point will have a different second derivative depending on which plane you take it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the opposite direction it will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
====Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r1 = r2 (and p1=p2=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r1=r2) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
====Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
translational energy=0 but not the vibrational&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the left. By contrast, the dynamic plot shows how the trajectory to the product oscillates as it takes into account the vibrational energies.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demostrating how the momentum of the system is constant regardless of the values you input for p1 and p2. However, the moemntum is seen to change with a dynamic plot as although it takes the translation energy = 0 (i.e. p1=p2=0), it accounts for the vibrational energies of the molecules.&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956||Not Reactive|| ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-84.956||Reactive || ||[[File:Trajectory_5_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;1st rxn (Exothermic):&#039;&#039;&#039; TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB). i.e. BC&amp;lt;AB&lt;br /&gt;
&lt;br /&gt;
H-H (BC) bond distance= 0.745 A&lt;br /&gt;
H-F (AB) bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;2nd rxn (Endo):&#039;&#039;&#039;TS will resemble the products as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-F (BC) is larger than that between the products i.e. H-H (AB). i.e. BC&amp;gt;AB (shown by Distance vs Time graph).&lt;br /&gt;
&lt;br /&gt;
H-F (BC) bond distance= 1.812 A&lt;br /&gt;
H-H (AB) bond distance= 0.745 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSendo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSendo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F.&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Distvstime_TSendo.png&amp;diff=791408</id>
		<title>File:Distvstime TSendo.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Distvstime_TSendo.png&amp;diff=791408"/>
		<updated>2019-05-23T17:23:38Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contourplot_TSendo.png&amp;diff=791404</id>
		<title>File:Contourplot TSendo.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contourplot_TSendo.png&amp;diff=791404"/>
		<updated>2019-05-23T17:22:30Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791373</id>
		<title>01354530estela</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=01354530estela&amp;diff=791373"/>
		<updated>2019-05-23T17:13:35Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==&#039;&#039;&#039;Molecular Reaction Dynamics&#039;&#039;&#039;==&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system&#039;&#039;&#039; ===&lt;br /&gt;
&lt;br /&gt;
====On a potential energy surface diagram, how is the transition state mathematically defined? How can the transition state be identified, and how can it be distinguished from a local minimum of the potential energy surface?====&lt;br /&gt;
&lt;br /&gt;
The transition state is formally defined as the maximum on the minimum energy path relating the reactants to products, mathematically this is defined by a saddle point which is not the same as a local maxima or minima. The transition state (saddle point) is therefore the point on the potential energy graph where the slopes in orthogonal directions are all opposite.  &lt;br /&gt;
&lt;br /&gt;
∂V(ri)/∂ri=0 for all three, i.e. the gradient of the potential = 0 for all three.&lt;br /&gt;
However, if you take partial derivatives you can differentiate between the three as a local minima, for instance, will always have a positive second derivative. By contrast, a saddle point will have a different second derivative depending on which plane you take it relative to i.e. the partial derivative in one direction will be a maxima (negative) and in the opposite direction it will be a minimum (positive).&lt;br /&gt;
&lt;br /&gt;
====Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with a “Internuclear Distances vs Time” plot for a relevant trajectory.====&lt;br /&gt;
&lt;br /&gt;
At the transitioin state r1 = r2 (and p1=p2=0) and there is no gradient at the directions perpendicular to the ridge. This can be used to find the position of the transition state using an internuclear vs time plot and looking for the distance (AB=BC; r1=r2) at which there are no oscillations nor direction towards the reactants or products. This distance was found to = 0.9078 A &lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSex1.png|frameless|450px|center]]&lt;br /&gt;
[[File:Animation 1.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
Note there is no overall release or absorption of energy as the reaction forms the same bond that is being broken and therefore the TS is exactly is the middle where AB=BC (follows hammond&#039;s postulate-&amp;gt; neither exo nor endo and so TS equally resembles the reactants as the products) and the reactants have the same energy as the products (shown by surface plot)&lt;br /&gt;
&lt;br /&gt;
====Comment on how the mep and the trajectory you just calculated differ.====&lt;br /&gt;
translational energy=0 but not the vibrational&lt;br /&gt;
&lt;br /&gt;
[[File:contourplot_mep.png|frameless|450px|center]]&lt;br /&gt;
[[File:contourplot_dynamics.png|frameless|450px|center]]&lt;br /&gt;
&lt;br /&gt;
From the contour plots of r1(BC)= 0.9179 and r2(AB)=0.9079 respectively, you can see how the trajectory greatly differs depending on whether you set the calculation type to dynamics or mep.&lt;br /&gt;
A Mep plot doesn&#039;t provide a realistic account of the motion of the atoms during the reaction as it takes the vibrational energy to = 0. As a result, you can see a straight line representing the trajectory on the graph on the left. By contrast, the dynamic plot shows how the trajectory to the product oscillates as it takes into account the vibrational energies.&lt;br /&gt;
The momenta vs time plots illustrate this concept more clearly by demostrating how the momentum of the system is constant regardless of the values you input for p1 and p2. However, the moemntum is seen to change with a dynamic plot as although it takes the translation energy = 0 (i.e. p1=p2=0), it accounts for the vibrational energies of the molecules.&lt;br /&gt;
&lt;br /&gt;
[[File:momentavstime_dynamics.png|frameless|350px|center]]   &lt;br /&gt;
[[File:Momentaplot2.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
====Complete the table above by adding the total energy, whether the trajectory is reactive or unreactive, and provide a plot of the trajectory and a small description for what happens along the trajectory. What can you conclude from the table?====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25 || -2.5  || -99.018|| Reactive|| ||&lt;br /&gt;
[[File:Trajectory_1_table.png|frameless|350px|center]] &lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.0  ||-100.456 ||Not Reactive || ||[[File:Trajectory_2_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5  || -2.5  ||-98.956 ||Reactive || ||[[File:Trajectory_3_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.0  ||-84.956||Not Reactive|| ||[[File:Trajectory_4_table.png|frameless|350px|center]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5  || -5.2  ||-84.956||Reactive || ||[[File:Trajectory_5_table.png|frameless|350px|center]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
====State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?====&lt;br /&gt;
&lt;br /&gt;
===&#039;&#039;&#039;EXERCISE 2: F-H-H system&#039;&#039;&#039;===&lt;br /&gt;
&lt;br /&gt;
====By inspecting the potential energy surfaces, classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?====&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;F+ H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ---&amp;gt; F-H + H&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-H (r1) bond distance= 0.74 A&lt;br /&gt;
H-F (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotexo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;br /&gt;
&lt;br /&gt;
The reactants (BC) are higher in energy than the products (AB) and therefore it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;H + H-F ---&amp;gt; H-H + F&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
H-F (r1) bond distance= 0.91 A&lt;br /&gt;
H-H (r2) bond distance= 2.3 A&lt;br /&gt;
p1=0 kg ms-1&lt;br /&gt;
p2=-2.7 kg ms-1&lt;br /&gt;
&lt;br /&gt;
[[File:Surfaceplotendo.png|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=H, B=H and C=F&lt;br /&gt;
&lt;br /&gt;
From the plot you can see the reactants (BC) are lower in energy than the products (AB) and therefore we can say the reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
Breaking bonds requires energy while making bonds releases energy.&lt;br /&gt;
This suggests that the H-F bond is stronger than the H-H bond as the reaction that results in its formation is exothermic, meaning the activation energy for breaking the H-H bond is small and therefore is compensated by the release of energy as a result of the H-F bond formation.&lt;br /&gt;
By contrast, the amount of energy you need to put into the system to break the H-F bond is greater than that released by the formation of the H-H bond, and so the second reaction is endothermic.&lt;br /&gt;
&lt;br /&gt;
====Locate the approximate position of the transition state.====&lt;br /&gt;
&lt;br /&gt;
Hammond&#039;s postulate:&lt;br /&gt;
&lt;br /&gt;
1st rxn (Exothermic): TS will resemble the reactants as they are closer in energy and therefore it will be located at a position where the distance between the reactants i.e. H-H (BC) is smaller than that of the products i.e. H-F (AB)&lt;br /&gt;
&lt;br /&gt;
H-H bond distance= 0.745 A&lt;br /&gt;
H-F bond distance= 1.812 A&lt;br /&gt;
p1=p2=0&lt;br /&gt;
&lt;br /&gt;
[[File:Contourplot_TSexo.png|frameless|350px|center]]&lt;br /&gt;
[[File:Distvstime_TSexo.png ‎|frameless|350px|center]]&lt;br /&gt;
&lt;br /&gt;
Where A=F, B=H and C=H.&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contourplot_TSex1.png&amp;diff=791361</id>
		<title>File:Contourplot TSex1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contourplot_TSex1.png&amp;diff=791361"/>
		<updated>2019-05-23T17:07:58Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Distvstime_TSexo.png&amp;diff=791357</id>
		<title>File:Distvstime TSexo.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Distvstime_TSexo.png&amp;diff=791357"/>
		<updated>2019-05-23T17:06:55Z</updated>

		<summary type="html">&lt;p&gt;El917: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>El917</name></author>
	</entry>
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