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		<title>MRD:chengwang01492455</title>
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		<updated>2020-05-08T22:48:20Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
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-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
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[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
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(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
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[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
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&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
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No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
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Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
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Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
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[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
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&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
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&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, it does not cross the transition barrier, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(has cross the transition barrier), But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
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&#039;&#039;&#039;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;
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The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
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&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
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&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
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&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
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&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
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Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. surface plot D, it initially forming the new molecule HAHB(reactants have crossed transition barrier), but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
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Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
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Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
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=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
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&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
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F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen from the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore reaction H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
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According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic. r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;will be shorter in length.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.&lt;br /&gt;
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Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
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[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
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&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
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Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
[[File:contourvb.png|250px|thumb|left|contour plot showing high vibration energy of products]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
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&lt;br /&gt;
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Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone in the IR, when system generate the products, in this reaction, HF, most of population is in the vibrational ground state, while some is in the 1st vibrational excited state. So it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number but lower intensity. 0 to 1 transition will be more intense, while intensity of overtone will decrease when taking snapshot overtime.&lt;br /&gt;
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&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in the reaction with early barrier.&lt;br /&gt;
&lt;br /&gt;
Exothermic reaction(early transition state): F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants with lower vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph a,b,c, as the vibrational energy(Higher HH momentum) given to reactants increase, the ease of reactive trajectory will decrease.&lt;br /&gt;
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Endothermic reaction(late transition state):H+HF, the reactants with higher vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph e,f,g, as the vibrational energy(Higher HF momentum) given to reactants increase, the ease of reactive trajectory will increase.&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{|-&lt;br /&gt;
|[[File:0.288.png|250px|thumb|a.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.2]]||[[File:0.7x.png|250px|thumb|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.7]]||[[File:1.5x.png|250px|thumb|c.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 1.5]]&lt;br /&gt;
|-&lt;br /&gt;
|[[File:5z.png|250px|thumb|e.rHH=140 pm rFH=74 pm, pFH= -0.2, pHH = 5]]||[[File:3z.png|250px|thumb|f.rHH=140 pm rFH=74 pm, pFH=-3 , pHH = 2]] ||[[File:10zz.png|250px|thumb|g.rHH=140 pm rFH=74 pm, pFH= 10, pHH = -0.2]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801258</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801258"/>
		<updated>2020-05-08T22:39:37Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, it does not cross the transition barrier, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(has cross the transition barrier), But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. surface plot D, it initially forming the new molecule HAHB(reactants have crossed transition barrier), but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen from the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore reaction H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
[[File:contourvb.png|250px|thumb|left|contour plot showing high vibration energy of products]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone in the IR, when system generate the products, in this reaction, HF, most of population is in the vibrational ground state, while some is in the 1st vibrational excited state. So it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number but lower intensity. 0 to 1 transition will be more intense, while intensity of overtone will decrease when taking snapshot overtime.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in the reaction with early barrier.&lt;br /&gt;
&lt;br /&gt;
Exothermic reaction(early transition state): F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants with lower vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph a,b,c, as the vibrational energy(Higher HH momentum) given to reactants increase, the ease of reactive trajectory will decrease.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Endothermic reaction(late transition state):H+HF, the reactants with higher vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph e,f,g, as the vibrational energy(Higher HF momentum) given to reactants increase, the ease of reactive trajectory will increase.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{|-&lt;br /&gt;
|[[File:0.288.png|250px|thumb|a.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.2]]||[[File:0.7x.png|250px|thumb|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.7]]||[[File:1.5x.png|250px|thumb|c.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 1.5]]&lt;br /&gt;
|-&lt;br /&gt;
|[[File:5z.png|250px|thumb|e.rHH=140 pm rFH=74 pm, pFH= -0.2, pHH = 5]]||[[File:3z.png|250px|thumb|f.rHH=140 pm rFH=74 pm, pFH=-3 , pHH = 2]] ||[[File:10zz.png|250px|thumb|g.rHH=140 pm rFH=74 pm, pFH= 10, pHH = -0.2]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801224</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801224"/>
		<updated>2020-05-08T22:19:02Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, it does not cross the transition barrier, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(has cross the transition barrier), But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. surface plot D, it initially forming the new molecule HAHB(reactants have crossed transition barrier), but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen from the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore reaction H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
[[File:contourvb.png|250px|thumb|left|contour plot showing high vibration energy of products]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone, the molecules will located in the ground state and also 1st exicited state, so it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in the reaction with early barrier.&lt;br /&gt;
&lt;br /&gt;
Exothermic reaction(early transition state): F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants with lower vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph a,b,c, as the vibrational energy(Higher HH momentum) given to reactants increase, the ease of reactive trajectory will decrease.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Endothermic reaction(late transition state):H+HF, the reactants with higher vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph e,f,g, as the vibrational energy(Higher HF momentum) given to reactants increase, the ease of reactive trajectory will increase.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{|-&lt;br /&gt;
|[[File:0.288.png|250px|thumb|a.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.2]]||[[File:0.7x.png|250px|thumb|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.7]]||[[File:1.5x.png|250px|thumb|c.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 1.5]]&lt;br /&gt;
|-&lt;br /&gt;
|[[File:5z.png|250px|thumb|e.rHH=140 pm rFH=74 pm, pFH= -0.2, pHH = 5]]||[[File:3z.png|250px|thumb|f.rHH=140 pm rFH=74 pm, pFH=-3 , pHH = 2]] ||[[File:10zz.png|250px|thumb|g.rHH=140 pm rFH=74 pm, pFH= 10, pHH = -0.2]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801221</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801221"/>
		<updated>2020-05-08T22:17:07Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, it does not cross the transition barrier, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(has cross the transition barrier), But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen from the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore reaction H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
[[File:contourvb.png|250px|thumb|left|contour plot showing high vibration energy of products]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone, the molecules will located in the ground state and also 1st exicited state, so it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in the reaction with early barrier.&lt;br /&gt;
&lt;br /&gt;
Exothermic reaction(early transition state): F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants with lower vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph a,b,c, as the vibrational energy(Higher HH momentum) given to reactants increase, the ease of reactive trajectory will decrease.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Endothermic reaction(late transition state):H+HF, the reactants with higher vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph e,f,g, as the vibrational energy(Higher HF momentum) given to reactants increase, the ease of reactive trajectory will increase.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{|-&lt;br /&gt;
|[[File:0.288.png|250px|thumb|a.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.2]]||[[File:0.7x.png|250px|thumb|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.7]]||[[File:1.5x.png|250px|thumb|c.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 1.5]]&lt;br /&gt;
|-&lt;br /&gt;
|[[File:5z.png|250px|thumb|e.rHH=140 pm rFH=74 pm, pFH= -0.2, pHH = 5]]||[[File:3z.png|250px|thumb|f.rHH=140 pm rFH=74 pm, pFH=-3 , pHH = 2]] ||[[File:10zz.png|250px|thumb|g.rHH=140 pm rFH=74 pm, pFH= 10, pHH = -0.2]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801220</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801220"/>
		<updated>2020-05-08T22:14:40Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen from the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore reaction H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
[[File:contourvb.png|250px|thumb|left|contour plot showing high vibration energy of products]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone, the molecules will located in the ground state and also 1st exicited state, so it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in the reaction with early barrier.&lt;br /&gt;
&lt;br /&gt;
Exothermic reaction(early transition state): F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants with lower vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph a,b,c, as the vibrational energy(Higher HH momentum) given to reactants increase, the ease of reactive trajectory will decrease.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Endothermic reaction(late transition state):H+HF, the reactants with higher vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph e,f,g, as the vibrational energy(Higher HF momentum) given to reactants increase, the ease of reactive trajectory will increase.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{|-&lt;br /&gt;
|[[File:0.288.png|250px|thumb|a.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.2]]||[[File:0.7x.png|250px|thumb|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.7]]||[[File:1.5x.png|250px|thumb|c.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 1.5]]&lt;br /&gt;
|-&lt;br /&gt;
|[[File:5z.png|250px|thumb|e.rHH=140 pm rFH=74 pm, pFH= -0.2, pHH = 5]]||[[File:3z.png|250px|thumb|f.rHH=140 pm rFH=74 pm, pFH=-3 , pHH = 2]] ||[[File:10zz.png|250px|thumb|g.rHH=140 pm rFH=74 pm, pFH= 10, pHH = -0.2]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contourvb.png&amp;diff=801217</id>
		<title>File:Contourvb.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Contourvb.png&amp;diff=801217"/>
		<updated>2020-05-08T22:12:03Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801215</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801215"/>
		<updated>2020-05-08T22:11:27Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen from the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore reaction H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
[[File:contourvb.png|250px|thumb|contour plot showing high vibration energy of products]]&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone, the molecules will located in the ground state and also 1st exicited state, so it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in the reaction with early barrier.&lt;br /&gt;
&lt;br /&gt;
Exothermic reaction(early transition state): F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants with lower vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph a,b,c, as the vibrational energy(Higher HH momentum) given to reactants increase, the ease of reactive trajectory will decrease.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Endothermic reaction(late transition state):H+HF, the reactants with higher vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph e,f,g, as the vibrational energy(Higher HF momentum) given to reactants increase, the ease of reactive trajectory will increase.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{|-&lt;br /&gt;
|[[File:0.288.png|250px|thumb|a.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.2]]||[[File:0.7x.png|250px|thumb|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.7]]||[[File:1.5x.png|250px|thumb|c.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 1.5]]&lt;br /&gt;
|-&lt;br /&gt;
|[[File:5z.png|250px|thumb|e.rHH=140 pm rFH=74 pm, pFH= -0.2, pHH = 5]]||[[File:3z.png|250px|thumb|f.rHH=140 pm rFH=74 pm, pFH=-3 , pHH = 2]] ||[[File:10zz.png|250px|thumb|g.rHH=140 pm rFH=74 pm, pFH= 10, pHH = -0.2]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801209</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801209"/>
		<updated>2020-05-08T22:06:52Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen from the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore reaction H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone, the molecules will located in the ground state and also 1st exicited state, so it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in the reaction with early barrier.&lt;br /&gt;
&lt;br /&gt;
Exothermic reaction(early transition state): F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants with lower vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph a,b,c, as the vibrational energy(Higher HH momentum) given to reactants increase, the ease of reactive trajectory will decrease.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Endothermic reaction(late transition state):H+HF, the reactants with higher vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph e,f,g, as the vibrational energy(Higher HF momentum) given to reactants increase, the ease of reactive trajectory will increase.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{|-&lt;br /&gt;
|[[File:0.288.png|250px|thumb|a.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.2]]||[[File:0.7x.png|250px|thumb|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.7]]||[[File:1.5x.png|250px|thumb|c.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 1.5]]&lt;br /&gt;
|-&lt;br /&gt;
|[[File:5z.png|250px|thumb|e.rHH=140 pm rFH=74 pm, pFH= -0.2, pHH = 5]]||[[File:3z.png|250px|thumb|f.rHH=140 pm rFH=74 pm, pFH=-3 , pHH = 2]] ||[[File:10zz.png|250px|thumb|g.rHH=140 pm rFH=74 pm, pFH= 10, pHH = -0.2]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801205</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801205"/>
		<updated>2020-05-08T22:05:38Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen from the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore reaction H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone, the molecules will located in the ground state and also 1st exicited state, so it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in the reaction with early barrier.&lt;br /&gt;
&lt;br /&gt;
Exothermic reaction(early barrier): F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants with lower vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph a,b,c, as the vibrational energy(Higher HH momentum) given to reactants increase, the ease of reactive trajectory will decrease.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Endothermic reaction(late barrier):H+HF, the reactants with higher vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph e,f,g, as the vibrational energy(Higher HF momentum) given to reactants increase, the ease of reactive trajectory will increase.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{|-&lt;br /&gt;
|[[File:0.288.png|250px|thumb|a.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.2]]||[[File:0.7x.png|250px|thumb|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.7]]||[[File:1.5x.png|250px|thumb|c.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 1.5]]&lt;br /&gt;
|-&lt;br /&gt;
|[[File:5z.png|250px|thumb|e.rHH=140 pm rFH=74 pm, pFH= -0.2, pHH = 5]]||[[File:3z.png|250px|thumb|f.rHH=140 pm rFH=74 pm, pFH=-3 , pHH = 2]] ||[[File:10zz.png|250px|thumb|g.rHH=140 pm rFH=74 pm, pFH= 10, pHH = -0.2]]&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801194</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801194"/>
		<updated>2020-05-08T21:57:12Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen from the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore reaction H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone, the molecules will located in the ground state and also 1st exicited state, so it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in the reaction with early barrier.&lt;br /&gt;
&lt;br /&gt;
Exothermic reaction(early barrier): F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants with lower vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph a,b,c, as the vibrational energy(Higher HH momentum) given to reactants increase, the ease of reactive trajectory will decrease.&lt;br /&gt;
&lt;br /&gt;
[[File:0.288.png|250px|thumb|a.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.2]][[File:0.7x.png|250px|thumb|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.7]][[File:1.5x.png|250px|thumb|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 1.5]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Endothermic reaction(late barrier):H+HF, the reactants with higher vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
&lt;br /&gt;
From graph e,f,g, as the vibrational energy(Higher HF momentum) given to reactants increase, the ease of reactive trajectory will increase.&lt;br /&gt;
&lt;br /&gt;
[[File:5z.png|250px|thumb|e.rHH=140 pm rFH=74 pm, pFH= -0.2, pHH = 5]][[File:3z.png|250px|thumb|f.rHH=140 pm rFH=74 pm, pFH=-3 , pHH = 2]][[File:10zz.png|250px|thumb|g.rHH=140 pm rFH=74 pm, pFH= 10, pHH = -0.2]]&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801193</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801193"/>
		<updated>2020-05-08T21:55:54Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
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[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
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&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen from the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore reaction H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
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[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
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&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone, the molecules will located in the ground state and also 1st exicited state, so it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in the reaction with early barrier.&lt;br /&gt;
&lt;br /&gt;
Exothermic reaction(early barrier): F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants with lower vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
From graph a,b,c, as the vibrational energy(Higher HH momentum) given to reactants increase, the ease of reactive trajectory will decrease.&lt;br /&gt;
&lt;br /&gt;
[[File:0.288.png|250px|thumb|a.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.2]][[File:0.7x.png|250px|thumb|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.7]][[File:1.5x.png|250px|thumb|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 1.5]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Endothermic reaction(late barrier):H+HF, the reactants with higher vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
From graph e,f,g, as the vibrational energy(Higher HF momentum) given to reactants increase, the ease of reactive trajectory will increase.&lt;br /&gt;
&lt;br /&gt;
[[File:5z.png|250px|thumb|e.rHH=140 pm rFH=74 pm, pFH= -0.2, pHH = 5]][[File:3z.png|250px|thumb|f.rHH=140 pm rFH=74 pm, pFH=-3 , pHH = 2]][[File:10zz.png|250px|thumb|g.rHH=140 pm rFH=74 pm, pFH= 10, pHH = -0.2]]&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
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		<updated>2020-05-08T21:53:50Z</updated>

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		<updated>2020-05-08T21:53:30Z</updated>

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		<updated>2020-05-08T21:52:34Z</updated>

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		<updated>2020-05-08T21:52:19Z</updated>

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		<updated>2020-05-08T21:52:03Z</updated>

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		<updated>2020-05-08T21:51:48Z</updated>

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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801180</id>
		<title>MRD:chengwang01492455</title>
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		<updated>2020-05-08T21:50:54Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen from the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore reaction H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone, the molecules will located in the ground state and also 1st exicited state, so it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in the reaction with early barrier.&lt;br /&gt;
&lt;br /&gt;
Exothermic reaction(early barrier): F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants with lower vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
From graph a,b,c, as the vibrational energy(Higher HH momentum) given to reactants increase, the ease of reactive trajectory will decrease.&lt;br /&gt;
&lt;br /&gt;
[[File:0.288.png|250px|thumb|left|a.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.2]][[File:0.7x.png|250px|thumb|center|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.7]][[File:1.5x.png|250px|thumb|right|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 1.5]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Endothermic reaction(late barrier):H+HF, the reactants with higher vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
From graph e,f,g, as the vibrational energy(Higher HF momentum) given to reactants increase, the ease of reactive trajectory will increase.&lt;br /&gt;
&lt;br /&gt;
[[File:5z.png|250px|thumb|left|e.rHH=140 pm rFH=74 pm, pFH= -0.2, pHH = 5]][[File:3z.png|250px|thumb|center|f.rHH=140 pm rFH=74 pm, pFH=-3 , pHH = 2]][[File:10zz.png|250px|thumb|right|g.rHH=140 pm rFH=74 pm, pFH= 10, pHH = -0.2]]&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801179</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801179"/>
		<updated>2020-05-08T21:49:52Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen from the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore reaction H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone, the molecules will located in the ground state and also 1st exicited state, so it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in the reaction with early barrier.&lt;br /&gt;
&lt;br /&gt;
Exothermic reaction(early barrier): F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the reactants with lower vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
From graph a,b,c, as the vibrational energy(Higher HH momentum) given to reactants increase, the ease of reactive trajectory will decrease.&lt;br /&gt;
&lt;br /&gt;
[[File:0.288.png|250px|thumb|left|a.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.2]][[File:0.7x.png|250px|thumb|center|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 0.7]][[File:1.5x.png|250px|thumb|right|b.rHH=74 pm rFH=170 pm, pFH= -1.6, pHH = 1.5]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Endothermic reaction(late barrier):H+HF, the reactants with higher vibrational energy could result in high possibility of reactive trajectory.&lt;br /&gt;
From graph e,f,g, as the vibrational energy(Higher HF momentum) given to reactants increase, the ease of reactive trajectory will increase.&lt;br /&gt;
&lt;br /&gt;
[[File:5z.png|250px|thumb|left|a.rHH=140 pm rFH=74 pm, pFH= -0.2, pHH = 5]][[File:3z.png|250px|thumb|center|b.rHH=140 pm rFH=74 pm, pFH=-3 , pHH = 2]][[File:10z.png|250px|thumb|right|b.rHH=140 pm rFH=74 pm, pFH= 10, pHH = -0.2]]&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801126</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801126"/>
		<updated>2020-05-08T20:55:56Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique can be used to monitor the emission of infrared radiation form the sample.&lt;br /&gt;
&lt;br /&gt;
The other method is to monitor the overtone, the molecules will located in the ground state and also 1st exicited state, so it is expected to see the intense 0 to 1 transition, and 1-2 overtone located in higher wave number.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Polanyi principle states that translational energy is more effective than vibrational energy in promoting an early-barrier.&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801070</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801070"/>
		<updated>2020-05-08T20:23:46Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Chemiluminescence techique  be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801040</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801040"/>
		<updated>2020-05-08T20:06:45Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:HFdistance.png&amp;diff=801032</id>
		<title>File:HFdistance.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:HFdistance.png&amp;diff=801032"/>
		<updated>2020-05-08T20:04:12Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Surface_PlotHF1.png&amp;diff=801031</id>
		<title>File:Surface PlotHF1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Surface_PlotHF1.png&amp;diff=801031"/>
		<updated>2020-05-08T20:03:54Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801026</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801026"/>
		<updated>2020-05-08T19:57:25Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm.  &lt;br /&gt;
&lt;br /&gt;
Transition state can be confirmed by examining its eigenvalue of hessian(one negative and one positive) and interneclear distance vs time plot (no oscillation) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801022</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=801022"/>
		<updated>2020-05-08T19:53:06Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference from: Laidler, Keith J, Chemical kinetics,pp. 88-98)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800998</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800998"/>
		<updated>2020-05-08T19:38:30Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|250px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Conclude from the table&#039;&#039;&#039;&lt;br /&gt;
From the table, smaller p1/p2 ratio will result in higher possibility of reactive trajectory. Higher value of momentum will result in more complicated trajectory, its energy will also more likely towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:&amp;lt;ref name=&amp;quot;LazyDog&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
=reference=&lt;br /&gt;
&amp;lt;ref name=&amp;quot;LazyDog&amp;quot;&amp;gt; Laidler, Keith J,&#039;&#039;Chemical kinetics&#039;&#039;pp. 88-98&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800986</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800986"/>
		<updated>2020-05-08T19:30:13Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]]&lt;br /&gt;
&lt;br /&gt;
[[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|250px|thumb|left|Internuclear Distances vs Time]]&lt;br /&gt;
&lt;br /&gt;
[[File:AB+1m.png|250px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|250px|thumb|left|Internuclear Distances vs Time]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1M.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|200px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800981</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800981"/>
		<updated>2020-05-08T19:27:43Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|300px|thumb|left|center|Internuclear Distances vs Time]][[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Conclusion from the table]]&lt;br /&gt;
Larger value of momentum will result in more complicated reaction trajectory, smaller value of p1/p2 will result in higher possibility of reactive trajectory. Also when both momentum is large, the Etotal will be more towards positive value.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:&amp;lt;ref name=&amp;quot;LazyDog&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=reference=&lt;br /&gt;
&amp;lt;ref name=&amp;quot;LazyDog&amp;quot;&amp;gt;Laidler, Keith J.&#039;&#039;Chemical kinetics&#039;&#039;pp. 88-98 &amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800951</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800951"/>
		<updated>2020-05-08T19:11:03Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]][[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|300px|thumb|left|Internuclear Distances vs Time]][[File:AB+1m.png|300px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|300px|thumb|left|Internuclear Distances vs Time]] [[File:BC+1M.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|300px|thumb|left|center|Internuclear Distances vs Time]][[File:finalposition.png|300px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800947</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800947"/>
		<updated>2020-05-08T19:09:38Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
(Figure 3) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
Wavy line was seen in dynamics trajectory where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
No vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
Velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]]&lt;br /&gt;
&lt;br /&gt;
[[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|250px|thumb|left|Internuclear Distances vs Time]]&lt;br /&gt;
&lt;br /&gt;
[[File:AB+1m.png|250px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|250px|thumb|left|Internuclear Distances vs Time]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1M.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
Set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm,&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1 &amp;lt;/sup&amp;gt;p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|200px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800940</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800940"/>
		<updated>2020-05-08T19:04:08Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.jpg|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
As its “Internuclear Distances vs Time”plot (Figure 1) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
wavy line was seen in dynamics trajectory，where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
no vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]]&lt;br /&gt;
&lt;br /&gt;
[[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|250px|thumb|left|Internuclear Distances vs Time]]&lt;br /&gt;
&lt;br /&gt;
[[File:AB+1m.png|250px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|250px|thumb|left|Internuclear Distances vs Time]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1M.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
when swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm&lt;br /&gt;
r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|200px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800935</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800935"/>
		<updated>2020-05-08T19:01:56Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.png|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
As its “Internuclear Distances vs Time”plot (Figure 1) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
wavy line was seen in dynamics trajectory，where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
no vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]]&lt;br /&gt;
&lt;br /&gt;
[[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|250px|thumb|left|Internuclear Distances vs Time]]&lt;br /&gt;
&lt;br /&gt;
[[File:AB+1m.png|250px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|250px|thumb|left|Internuclear Distances vs Time]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1M.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
when swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm&lt;br /&gt;
r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|200px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800928</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800928"/>
		<updated>2020-05-08T19:00:27Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatecc.png|thumb|center|Figure 1.surface plot of transition state]]&lt;br /&gt;
&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
As its “Internuclear Distances vs Time”plot (Figure 1) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
wavy line was seen in dynamics trajectory，where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
no vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]]&lt;br /&gt;
&lt;br /&gt;
[[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|250px|thumb|left|Internuclear Distances vs Time]]&lt;br /&gt;
&lt;br /&gt;
[[File:AB+1m.png|250px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|250px|thumb|left|Internuclear Distances vs Time]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1M.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
when swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm&lt;br /&gt;
r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|200px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Transitionstatecc.jpg&amp;diff=800927</id>
		<title>File:Transitionstatecc.jpg</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Transitionstatecc.jpg&amp;diff=800927"/>
		<updated>2020-05-08T18:59:30Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: Cw1018 uploaded a new version of File:Transitionstatecc.jpg&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Eigenvalues.png&amp;diff=800907</id>
		<title>File:Eigenvalues.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Eigenvalues.png&amp;diff=800907"/>
		<updated>2020-05-08T18:45:08Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800899</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800899"/>
		<updated>2020-05-08T18:41:04Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
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-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
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-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
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Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
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[[File:transitionstatecc.png|thumb|center|Figure 1.surface plot of transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.hessian plot on transition state]]&lt;br /&gt;
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&#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;
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H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
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Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
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At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
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The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
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As its “Internuclear Distances vs Time”plot (Figure 1) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
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[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
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&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
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The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
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Difference:&lt;br /&gt;
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wavy line was seen in dynamics trajectory，where there is smooth and shorter path shown in mep. &lt;br /&gt;
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no vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
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velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
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Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
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[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]]&lt;br /&gt;
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[[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
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&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|250px|thumb|left|Internuclear Distances vs Time]]&lt;br /&gt;
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[[File:AB+1m.png|250px|thumb|center|Momenta vs Time]]&lt;br /&gt;
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r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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[[File:BC+1D.png|250px|thumb|left|Internuclear Distances vs Time]] &lt;br /&gt;
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[[File:BC+1M.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
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when swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm&lt;br /&gt;
r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
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[[File:finalpositionin.png|200px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
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&#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;
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{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
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&#039;&#039;&#039;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;
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The main assumption of transition state theory states:(reference)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
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Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
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=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
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&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
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F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
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Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
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It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
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According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
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Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
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[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
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&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
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Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
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The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
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r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
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Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
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r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
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Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&lt;br /&gt;
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&#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;
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From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
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&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Transitionstatecc.jpg&amp;diff=800895</id>
		<title>File:Transitionstatecc.jpg</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Transitionstatecc.jpg&amp;diff=800895"/>
		<updated>2020-05-08T18:39:45Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800888</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800888"/>
		<updated>2020-05-08T18:36:04Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0. It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever. In addition, according to the Hammond&#039;s postulate, if reaction is exothermic, the transition state will resemble the reactants, while if the reaction is endothermic, it will resemble the products.                                                                  &lt;br /&gt;
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-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
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Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive (positive curvature). &lt;br /&gt;
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[[File:transitionstatewc.png|thumb|center|Figure 1.transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.]]&lt;br /&gt;
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&#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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, According to Hammond&#039;s postulate transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.775 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The eigenvalues of hessian show one positive and one negative (Figure 2).&lt;br /&gt;
&lt;br /&gt;
As its “Internuclear Distances vs Time”plot (Figure 1) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are no longer oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 3“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
wavy line was seen in dynamics trajectory，where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
no vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]]&lt;br /&gt;
&lt;br /&gt;
[[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|250px|thumb|left|Internuclear Distances vs Time]]&lt;br /&gt;
&lt;br /&gt;
[[File:AB+1m.png|250px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|250px|thumb|left|Internuclear Distances vs Time]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1M.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
when swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm&lt;br /&gt;
r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|200px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800867</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800867"/>
		<updated>2020-05-08T18:12:06Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0 , It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive(curvature positive). &lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatewc.png|thumb|center|Figure 1.transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric,transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.773 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
As its “Internuclear Distances vs Time”plot (Figure 1) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are not oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 1“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
wavy line was seen in dynamics trajectory，where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
no vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]]&lt;br /&gt;
&lt;br /&gt;
[[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|250px|thumb|left|Internuclear Distances vs Time]]&lt;br /&gt;
&lt;br /&gt;
[[File:AB+1m.png|250px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|250px|thumb|left|Internuclear Distances vs Time]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1M.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
when swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm&lt;br /&gt;
r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|200px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but HB will go back to HC,the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
The main assumption of transition state theory states:(reference)&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule again.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
Assumption &amp;lt;1&amp;gt; will overestimate the rate. In TST, it count anythings across the activation barrier,but in real reaction, there is presence of recrossing, the products could reform the reactants, no reaction is happened, e.g. in Figure _, it initially forming the new molecule HAHB, but HB will go back to HC, forming reactants HCHB agian.&lt;br /&gt;
Assumption &amp;lt;4&amp;gt; will underestimate the rate. There is presence of tunneling effect in real reaction, especially for light molecules, they don&#039;t need to go over high activation energy.&lt;br /&gt;
Generally, recrossing is more significant than tunneling effect, TST overestimate the rate.&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic.&lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&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;
From the reactants to products, the small vibrational and tranlational energy will give rise to large vibrational and translational energy. Energy will release in two ways:&lt;br /&gt;
&amp;lt;1&amp;gt; vibrational kinetic energy of products &lt;br /&gt;
&amp;lt;2&amp;gt; translational kinetic energy of products&lt;br /&gt;
Both of them will generate heat( vibrational energy will release as vibratioanl relaxation which given off infrared radiation as heat).Bond calorimetry could measure the total heat release as it will cause temperature rises of outer system.&lt;br /&gt;
Vibronic spectroscopy can be used to monitor the release of vibrational energy by analysing its emission spectra.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.&#039;&#039;&#039;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800603</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800603"/>
		<updated>2020-05-08T14:16:33Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surface,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0 , It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
Hessian at the point can also be used to distinguish transition state from the local minimum. At transition state, It will have negative eigenvalues of hessian along one direction (In Figure, red line), while positive eigenvalues of hessian along the direction orthogonal to the previous one(In Figure, blue line). At local minima, hessian will always be positive defined with all eigenvalues are positive(curvature positive). &lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatewc.png|thumb|center|Figure 1.transition state]]&lt;br /&gt;
[[File:eigenvalues.png|thumb|center|Figure 2.]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric,transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.773 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
As its “Internuclear Distances vs Time”plot (Figure 1) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are not oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 1“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
wavy line was seen in dynamics trajectory，where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
no vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]]&lt;br /&gt;
&lt;br /&gt;
[[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|250px|thumb|left|Internuclear Distances vs Time]]&lt;br /&gt;
&lt;br /&gt;
[[File:AB+1m.png|250px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|250px|thumb|left|Internuclear Distances vs Time]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1M.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
when swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm&lt;br /&gt;
r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|200px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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 assumption of transition state theory states:&lt;br /&gt;
&amp;lt;1&amp;gt; molecules systems in direction of products cannot return back and form reactants molecule agian.&lt;br /&gt;
&amp;lt;2&amp;gt; The energy distribution among the reactants molecule is same as Boltzmann distribution.&lt;br /&gt;
&amp;lt;3&amp;gt; It is permissible to separate the motion of system over the col from the other other motions associated with the activated complex.&lt;br /&gt;
&amp;lt;4&amp;gt; A chemical reaction can be satisfactorily treated in terms of classical motions over the barrier, quantum effects being ignored.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic. &lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800521</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800521"/>
		<updated>2020-05-08T13:17:22Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surfac,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0 , It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatewc.png|thumb|center|Figure 1.transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric,transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.773 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
As its “Internuclear Distances vs Time”plot (Figure 1) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are not oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 1“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
wavy line was seen in dynamics trajectory，where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
no vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]]&lt;br /&gt;
&lt;br /&gt;
[[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|250px|thumb|left|Internuclear Distances vs Time]]&lt;br /&gt;
&lt;br /&gt;
[[File:AB+1m.png|250px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|250px|thumb|left|Internuclear Distances vs Time]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1M.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
when swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm&lt;br /&gt;
r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|200px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
&lt;br /&gt;
Therefore H + HF is endothermic, reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amount of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic. &lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:MepHF.png&amp;diff=800499</id>
		<title>File:MepHF.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:MepHF.png&amp;diff=800499"/>
		<updated>2020-05-08T12:52:34Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: Cw1018 uploaded a new version of File:MepHF.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800494</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800494"/>
		<updated>2020-05-08T12:50:32Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surfac,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0 , It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatewc.png|thumb|center|Figure 1.transition state]]&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;
&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric,transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.773 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
As its “Internuclear Distances vs Time”plot (Figure 1) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are not oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 1“Internuclear Distances vs Time” plot]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
wavy line was seen in dynamics trajectory，where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
no vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]]&lt;br /&gt;
&lt;br /&gt;
[[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|250px|thumb|left|Internuclear Distances vs Time]]&lt;br /&gt;
&lt;br /&gt;
[[File:AB+1m.png|250px|thumb|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|250px|thumb|left|Internuclear Distances vs Time]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1M.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
when swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm&lt;br /&gt;
r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|200px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
Therefore H + HF is endothermic,reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amountb of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic. &lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|energy vs time plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|energy vs time plot for mep simulation]]&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800489</id>
		<title>MRD:chengwang01492455</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:chengwang01492455&amp;diff=800489"/>
		<updated>2020-05-08T12:48:09Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;br /&gt;
= H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system=&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;
-- It is the saddle point in potential energy surfac,at this point the slope in all orthogonal directions are all zero, ∂V(ri)/∂ri=0 , It is the &#039;&#039;maximum&#039;&#039; on the minimum energy path linking reactants and the products(Figure 1). The point starts a trajectory exactly at the transition state, with no initial momentum, it will remain there forever.                                                                  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
-- The difference between local minimum and transition state :&lt;br /&gt;
The transition state is neither minimum or maximum.For local minima,its second derivative is always &amp;gt;0, while at transition state, because it is saddle point, the second partial derivative with respective to one axis is negative, while to another axis will be positive, which means at the transition state, it has local minima in one direction but local maxima in the other direction(orthogonal to previous one).&lt;br /&gt;
&lt;br /&gt;
[[File:transitionstatewc.png|thumb|center|Figure 1.transition state]]&lt;br /&gt;
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&#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;
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&lt;br /&gt;
H+ Hr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric,transition state will be 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 p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;): 90.773 pm&lt;br /&gt;
&lt;br /&gt;
At this symmetric transition state, as gradient of potential energy surfaces equals to zero, its initial forces are also 0 Kg.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
As its “Internuclear Distances vs Time”plot (Figure 1) illustrated, the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; will stay constant at certain value, meaning the atoms are not oscillating at this transition state.&lt;br /&gt;
&lt;br /&gt;
[[File:Animation22.png|thumb|center|Figure 1“Internuclear Distances vs Time” plot]]&lt;br /&gt;
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&#039;&#039;&#039;Comment on how the &#039;&#039;mep&#039;&#039; and the trajectory you just calculated differ.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The reaction path mep is set with system is slightly displaced from the transition states (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm and the momenta 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 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
Difference:&lt;br /&gt;
&lt;br /&gt;
wavy line was seen in dynamics trajectory，where there is smooth and shorter path shown in mep. &lt;br /&gt;
&lt;br /&gt;
no vibrational energy for mep--not oscillating for mep. &lt;br /&gt;
&lt;br /&gt;
velocities are always reset to zero in each time step, so kinetic energy is zero in mep -- path is shorter than dynamic trajectory.&lt;br /&gt;
&lt;br /&gt;
Total energy in system is always constant in dynamics simulation, while total energy in system is decreased in mep (kinetic energy is always zero, while potential energy is decreased.)&lt;br /&gt;
&lt;br /&gt;
[[File:Anmep.png|thumb|left|Contour plot of mep trajectory]]&lt;br /&gt;
&lt;br /&gt;
[[File:Andy.png|thumb|center|Contour plot of dynamics trajectory]]&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;nowiki&amp;gt; &amp;lt;/nowiki&amp;gt;r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1 pm=91.775 pm,  r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm ,p1=p2=0&lt;br /&gt;
[[File:AB+1.png|250px|thumb|left|Internuclear Distances vs Time]]&lt;br /&gt;
&lt;br /&gt;
[[File:AB+1m.png|250px|thumb|center|Momenta vs Time]]&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;=90.775 pm, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;+1=91.775 pm. p1 = p2 = 0.0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1D.png|250px|thumb|left|Internuclear Distances vs Time]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:BC+1M.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
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&lt;br /&gt;
when swapping the initial condition of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. From the “Internuclear Distances vs Time”and “Momenta vs Time”, it can be seen &lt;br /&gt;
that the curve of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; swap the position,but remaining the same trend.&lt;br /&gt;
&lt;br /&gt;
set the initial position to final value of above trajectory(reverse the sign of final momentum)&lt;br /&gt;
r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=352.59 pm&lt;br /&gt;
r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=74.04 pm&lt;br /&gt;
p1=-5.07g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
p2=-3.20g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As the new plot shows the trajectory will initially return pack to the r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; =90.775 pm,r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 91.775 pm, no reaction takes place, the system will then return back to its initial position.&lt;br /&gt;
&lt;br /&gt;
[[File:finalpositionin.png|200px|thumb|left|center|Internuclear Distances vs Time]]&lt;br /&gt;
[[File:finalposition.png|250px|thumb|center|center|Momenta vs Time]]&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&#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;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  ||-414.28 ||Yes ||HC-HB + HA is the initial state. Initially(before collision), HA is steadily approaching HBHC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased with r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; almost same, trajectory crosses the transition state  After the collision, it will become HC+ HB-HA.HC is steadily leaving from HAHB, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; is constantly increasing||[[File:Surface_PlotA.png|200px|thumb|center|center|surface plotA]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  ||-420.77 ||No  || HC-HB + HA is the initial state. HA is steadily approaching HBhC,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; is steadily decreased. But the collision does not happen as HA haven&#039;t had enough kinetic energy to reach the HB, the trajectory will go back to initial state HC-HB + HA ||[[File:Surface_PlotB.png|200px|thumb|center|center|surface plotB]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  ||-413.977 || Yes ||Almost the same illustration in A, r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HC,new molecule HA-HB forms and it has higher vibrational frequency than plot A, r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; increases as C is leaving away ||[[File:Surface_PlotC.png|200px|thumb|center|center|surface plotC]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277 ||No||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away(the system cross transition state), but the trajectory finally goes back to reactant. ||[[File:Surface_PlotD.png|200px|thumb|center|center|surface plotD]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 ||-349.477 || Yes ||HC-HB + HA is the initial state,r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; decreases as HA approach HB-HB,HA collide with HB forms new HAHB with HC leaving away, But the molecule has very high vibrational energy, leading to HB approacth Hc again, the trajectory goes towards initial state, but then remaining strong momentum will force HB goes to HA again, the trajectory finally goes to HC+ HB-HA with HC leaving away ||[[File:Surface_PlotE.png|200px|thumb|center|center|surface plotE]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;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;
&lt;br /&gt;
=F - H - H system =&lt;br /&gt;
&#039;&#039;&#039;By inspecting the potential energy surfaces, classify the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?&lt;br /&gt;
Locate the approximate position of the transition state.&#039;&#039;&#039;&lt;br /&gt;
F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;: when the initial conditions is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;= 130 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74 pm, p&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=0 g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, p&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=-0.5g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, it can be seen fromn the surface plot that system will undergo reactive trajectory,reactants F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are higher in energy than the products H + HF, the total energy is negative at -440.229kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;. it indicates the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction is exothermic.&lt;br /&gt;
Therefore H + HF is endothermic,reactants H + HF are lower in energy than the products F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;.&lt;br /&gt;
It also states that the bond strength of H-F is stronger than H-H, so forming H-F bond release large amountb of the energy,resulting in exothermic reaction.&lt;br /&gt;
[[File:Surface_PlotHF1.png|300px|thumb|center|center|surface plotE]]&lt;br /&gt;
&lt;br /&gt;
According to Hammond&#039;s postulate, the transition state will more likely to resemble the reactants in  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction, because it&#039;s exothermic. &lt;br /&gt;
&lt;br /&gt;
Approximate position of transition state is r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=181.2 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;= 74.51 pm. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:HFcontourplot.png|300px|thumb|center|center|contour plot for transition state]]&lt;br /&gt;
[[File:HFdistance.png|300px|thumb|center|Internuclear distance vs time graph at transition state]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Report the activation energy for both reactions.&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Energy at transition state is -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Energy of reactants for F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; and H + HF using the same procedure as H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system. As transition state has been located, energy of reactants can be found by importing mep.&lt;br /&gt;
&lt;br /&gt;
The initial condition of the system was slightly displaced from transition state with zero momentum:&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;+ 1 pm = =182.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number(1000),size(0.3). Last geometry energy (r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=239.62 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=74.02 pm) was recorded at -435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for  F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction : -433.980 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;1.023 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
r&amp;lt;sub&amp;gt;FH &amp;lt;/sub&amp;gt; -1 pm = =180.2 pm,  r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt; = 74.51 pm, steps was set at number (1000),size (0.3). Last geometry(r&amp;lt;sub&amp;gt;FH&amp;lt;/sub&amp;gt;=92.00 pm, r&amp;lt;sub&amp;gt;HH&amp;lt;/sub&amp;gt;=274.29 pm) energy was recorded at -560.485 kJ.mol&amp;lt;sup&amp;gt;-1  &amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Activation energy for H + HF reaction : -560.485 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;-（-435.003 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;）= &#039;&#039;&#039;125.482 kJ.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
[[File:mepHF.png|300px|thumb|center|contour plot for mep simulation]][[File:mepHF2.png|300px|thumb|center|contour plot for mep simulation]]&lt;/div&gt;</summary>
		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:HF1.png&amp;diff=800486</id>
		<title>File:HF1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:HF1.png&amp;diff=800486"/>
		<updated>2020-05-08T12:38:49Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
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		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:MepHF.png&amp;diff=800485</id>
		<title>File:MepHF.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:MepHF.png&amp;diff=800485"/>
		<updated>2020-05-08T12:38:24Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
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		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:HFcontourplot.png&amp;diff=800484</id>
		<title>File:HFcontourplot.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:HFcontourplot.png&amp;diff=800484"/>
		<updated>2020-05-08T12:37:59Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
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		<author><name>Cw1018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:MepHF2.png&amp;diff=800483</id>
		<title>File:MepHF2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:MepHF2.png&amp;diff=800483"/>
		<updated>2020-05-08T12:37:07Z</updated>

		<summary type="html">&lt;p&gt;Cw1018: &lt;/p&gt;
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		<author><name>Cw1018</name></author>
	</entry>
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