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	<updated>2026-06-10T13:37:19Z</updated>
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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620710</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620710"/>
		<updated>2017-05-12T13:06:50Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Figure 1 shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). &lt;br /&gt;
&lt;br /&gt;
The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|Figure 1. Intermolecular Distance vs Time,r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0.74 Å, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=2.30 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.70]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure 2 shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|Figure 2. Intermolecular Distance vs Time with (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. &lt;br /&gt;
&lt;br /&gt;
The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
[[File:yls158.PNG|thumb|450px|none|Figure 3. Intermolecular Distance vs Time at the transition state]]&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Therefore;&lt;br /&gt;
&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Due to the conservation of energy the amount of energy given out should be the same magnitude as the amount of energy taken in by the reverse reaction of H-F + H. &lt;br /&gt;
&lt;br /&gt;
To confirm this experimentally, the reverse reaction of H-F + H should be carried out and the magnitude of the energy take in should be recorded then compared to the energy given out by the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;br /&gt;
Based on the Hammond&#039;s postulate, the exothermic reactions have early transition states. With the higher translational energy, the reactants can rearrange themselves to form the transition state more easily. Hence, higher reaction efficiency is achieved when there is more translational energy compared to vibrational energy.&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620707</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620707"/>
		<updated>2017-05-12T13:06:27Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Report the activation energy for both reactions. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Figure 1 shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). &lt;br /&gt;
&lt;br /&gt;
The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|Figure 1. Intermolecular Distance vs Time,r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0.74 Å, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=2.30 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.70]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure 2 shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|Figure 2. Intermolecular Distance vs Time with (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. &lt;br /&gt;
&lt;br /&gt;
The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
[[File:yls158.PNG|thumb|450px|none|Figure 3. Intermolecular Distance vs Time at the transition state]]&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
&lt;br /&gt;
Therefore;&lt;br /&gt;
&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Due to the conservation of energy the amount of energy given out should be the same magnitude as the amount of energy taken in by the reverse reaction of H-F + H. &lt;br /&gt;
&lt;br /&gt;
To confirm this experimentally, the reverse reaction of H-F + H should be carried out and the magnitude of the energy take in should be recorded then compared to the energy given out by the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;br /&gt;
Based on the Hammond&#039;s postulate, the exothermic reactions have early transition states. With the higher translational energy, the reactants can rearrange themselves to form the transition state more easily. Hence, higher reaction efficiency is achieved when there is more translational energy compared to vibrational energy.&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620701</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620701"/>
		<updated>2017-05-12T13:04:48Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure 1 shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|Figure 1. Intermolecular Distance vs Time,r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0.74 Å, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=2.30 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.70]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure 2 shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|Figure 2. Intermolecular Distance vs Time with (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
[[File:yls158.PNG|thumb|450px|none|Figure 3. Intermolecular Distance vs Time at the transition state]]&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
Therefore;&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Due to conservation of energy the amount of energy given out should be the same magnitude as the amount of energy taken in by the reverse reaction of H-F + H. To confirm this experimentally, the reverse reaction of H-F + H should be carried out and the&lt;br /&gt;
magnitude of the energy take in should be recorded then compared to the energy&lt;br /&gt;
given out by the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;br /&gt;
Based on the Hammond&#039;s postulate, the exothermic reactions have early transition states. With the higher translational energy, the reactants can rearrange themselves to form the transition state more easily. Hence, higher reaction efficiency is achieved when there is more translational energy compared to vibrational energy.&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620643</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620643"/>
		<updated>2017-05-12T12:52:13Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally? */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure 1 shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|Figure 1. Intermolecular Distance vs Time,r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0.74 Å, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=2.30 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.70]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure 2 shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|Figure 2. Intermolecular Distance vs Time with (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
[[File:yls158.PNG|thumb|450px|none|Figure 3. Intermolecular Distance vs Time at the transition state]]&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
Therefore;&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic. Due to conservation of energy the amount of energy given out should be the same magnitude as the amount of energy taken in by the reverse reaction of H-F + H. To confirm this experimentally, the reverse reaction of H-F + H should be carried out and the&lt;br /&gt;
magnitude of the energy take in should be recorded then compared to the energy&lt;br /&gt;
given out by the F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; reaction.&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620632</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620632"/>
		<updated>2017-05-12T12:45:07Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Locate the approximate position of the transition state. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure 1 shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|Figure 1. Intermolecular Distance vs Time,r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0.74 Å, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=2.30 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.70]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure 2 shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|Figure 2. Intermolecular Distance vs Time with (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
[[File:yls158.PNG|thumb|450px|none|Figure 3. Intermolecular Distance vs Time at the transition state]]&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
Therefore;&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620631</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620631"/>
		<updated>2017-05-12T12:44:35Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Locate the approximate position of the transition state. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure 1 shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|Figure 1. Intermolecular Distance vs Time,r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0.74 Å, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=2.30 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.70]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure 2 shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|Figure 2. Intermolecular Distance vs Time with (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
[[File:yls158.PNG|thumb|450px|none|Figure 3. Intermolecular Distance vs Time]]&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
Therefore;&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620629</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620629"/>
		<updated>2017-05-12T12:43:44Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure 1 shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|Figure 1. Intermolecular Distance vs Time,r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0.74 Å, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=2.30 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.70]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure 2 shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|Figure 2. Intermolecular Distance vs Time with (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
[[File:yls158.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
Therefore;&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620626</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620626"/>
		<updated>2017-05-12T12:43:21Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure 1 shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|Figure 1. Intermolecular Distance vs Time,r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0.74 Å, rr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=2.30 Å, p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=0 pr&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=-2.70]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure 2 shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|Figure 2. Intermolecular Distance vs Time with (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
[[File:yls158.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
Therefore;&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620620</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620620"/>
		<updated>2017-05-12T12:42:08Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure 1 shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|Figure 1. Intermolecular Distance vs Time]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure 2 shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|Figure 2. Intermolecular Distance vs Time with (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
[[File:yls158.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
Therefore;&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620618</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620618"/>
		<updated>2017-05-12T12:41:03Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure 1 shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|Figure 1. Intermolecular Distance vs Time]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
[[File:yls158.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
Therefore;&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620616</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620616"/>
		<updated>2017-05-12T12:40:20Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Report your best estimate of the transition state position (rts) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|Figure 1. Intermolecular Distance vs Time]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
[[File:yls158.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
Therefore;&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620611</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620611"/>
		<updated>2017-05-12T12:38:44Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Locate the approximate position of the transition state. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
[[File:yls158.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
Therefore;&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls158.PNG&amp;diff=620609</id>
		<title>File:Yls158.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls158.PNG&amp;diff=620609"/>
		<updated>2017-05-12T12:38:28Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620607</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620607"/>
		<updated>2017-05-12T12:37:09Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Exercise 2: F - H - H system */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Report the activation energy for both reactions.===&lt;br /&gt;
&lt;br /&gt;
Potential Energy for the Transition State = -103.75 kcal/mol&lt;br /&gt;
Potential Energy for the H-H / F = -104.0kcal/mol&lt;br /&gt;
Potential Energy for the H-F / H = -133.7 kcal/mol&lt;br /&gt;
Therefore;&lt;br /&gt;
The activation energy for H + HF is +30.05 kcal/mol&lt;br /&gt;
The activation energy for F + H-H is +0.25 kcal/mol&lt;br /&gt;
&lt;br /&gt;
===In light of the fact that energy is conserved, discuss the mechanism of release of the reaction energy. How could this be confirmed experimentally?===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Discuss how the distribution of energy between different modes (translation and vibration) affect the efficiency of the reaction, and how this is influenced by the position of the transition state.===&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620606</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620606"/>
		<updated>2017-05-12T12:36:06Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Exercise 2: F - H - H system */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===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;
The reaction F + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where r&amp;lt;sub&amp;gt;H-F&amp;lt;/sub&amp;gt; = 1.813 Å and r&amp;lt;sub&amp;gt;H-H&amp;lt;/sub&amp;gt; = 0.744 Å which is similar to the bond length of H-H (reactants).&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620604</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620604"/>
		<updated>2017-05-12T12:34:49Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Exercise 2: F - H - H system */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;br /&gt;
&lt;br /&gt;
===Classify the F + H2 and H + HF reactions according to their energetics (endothermic or exothermic). How does this relate to the bond strength of the chemical species involved?===&lt;br /&gt;
&lt;br /&gt;
The reaction F + H2 is exothermic and H + HF is endothermic as the bond enthalpy of H-F is higher than H-H. &lt;br /&gt;
&lt;br /&gt;
===Locate the approximate position of the transition state.===&lt;br /&gt;
&lt;br /&gt;
According to Hammond’s postulate, in an exothermic reaction, the transition state resembles the reactants. &lt;br /&gt;
Therefore, the transition state exists where rH-F = 1.813 Å and rH-F = 0.744 Å which is similar to the bond length of H-H (reactants)&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620600</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620600"/>
		<updated>2017-05-12T12:32:42Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620599</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620599"/>
		<updated>2017-05-12T12:31:53Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yees&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunneling.&lt;br /&gt;
&lt;br /&gt;
== Exercise 2: F - H - H system ==&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620596</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620596"/>
		<updated>2017-05-12T12:30:00Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yees&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
Transition State Theory assumes that the motion of the atoms follows classical mechanics as the mass of electrons are negligible compared to the atoms. However, this assumption ignores quantum effects such as quantum tunnelling.&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620595</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620595"/>
		<updated>2017-05-12T12:29:18Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===State what are the main assumptions of Transition State Theory. Given the results you have obtained, how will Transition State Theory predictions for reaction rate values compare with experimental values?===&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yees&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620594</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620594"/>
		<updated>2017-05-12T12:28:23Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls152.PNG|thumb|450px|none|]]&lt;br /&gt;
&lt;br /&gt;
===Comment on how the mep and the trajectory you just calculated differ.===&lt;br /&gt;
&lt;br /&gt;
The minimum energy path (mep) always resets its velocity to zero. The trajectory follows the minima of the ‘valley’ towards the transition state. This gives a straight line trajectory where as in the dynamics calculations, the vibrational energies are considered so the trajectory by dynamic calculations follow an oscillating path.&lt;br /&gt;
&lt;br /&gt;
===Complete the table by adding a column reporting if the trajectory is reactive or unreactive. For each set of initial conditions, provide a screenshot of the trajectory and a small description for what happens along the trajectory.===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
! Does the reaction happen?&lt;br /&gt;
! Trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -1.25&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls153.PNG|thumb|The energy is enough for the atom to reach and pass through the transition state forming a B-C bond.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls154.PNG|thumb|&lt;br /&gt;
The energy is only enough for the atoms to approach to each other. Insufficient energy for the reaction to happen.]]&lt;br /&gt;
|-&lt;br /&gt;
| -1.5&lt;br /&gt;
| -2.5&lt;br /&gt;
| Yees&lt;br /&gt;
|[[File:yls155.PNG|thumb|The atoms have sufficient energy to pass through the transition state.&lt;br /&gt;
A bond is formed between B-C, which oscillates due to vibrations.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.0&lt;br /&gt;
| No&lt;br /&gt;
|[[File:yls156.PNG|thumb|The transition state is reached however it rolls back down towards the reactants.]]&lt;br /&gt;
|-&lt;br /&gt;
| -2.5&lt;br /&gt;
| -5.2&lt;br /&gt;
| Yes&lt;br /&gt;
|[[File:yls157.PNG|thumb|&lt;br /&gt;
The atoms pass through the transition state twice and the bond between B-C gets formed.]]&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls157.PNG&amp;diff=620591</id>
		<title>File:Yls157.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls157.PNG&amp;diff=620591"/>
		<updated>2017-05-12T12:23:37Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls156.PNG&amp;diff=620590</id>
		<title>File:Yls156.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls156.PNG&amp;diff=620590"/>
		<updated>2017-05-12T12:23:27Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls155.PNG&amp;diff=620589</id>
		<title>File:Yls155.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls155.PNG&amp;diff=620589"/>
		<updated>2017-05-12T12:23:10Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls154.PNG&amp;diff=620588</id>
		<title>File:Yls154.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls154.PNG&amp;diff=620588"/>
		<updated>2017-05-12T12:22:58Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls153.PNG&amp;diff=620587</id>
		<title>File:Yls153.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls153.PNG&amp;diff=620587"/>
		<updated>2017-05-12T12:22:48Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls152.PNG&amp;diff=620577</id>
		<title>File:Yls152.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls152.PNG&amp;diff=620577"/>
		<updated>2017-05-12T12:16:19Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620574</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620574"/>
		<updated>2017-05-12T12:13:38Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;br /&gt;
&lt;br /&gt;
[[File:yls151.PNG|thumb|]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls151.PNG&amp;diff=620573</id>
		<title>File:Yls151.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls151.PNG&amp;diff=620573"/>
		<updated>2017-05-12T12:13:08Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620565</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620565"/>
		<updated>2017-05-12T12:08:31Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131 Å at this point of intersection.&lt;br /&gt;
By testing different initial conditions where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;and p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; = 0, figure (X) shows the actual value of r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; is determined to be 0.908 Å&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620563</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620563"/>
		<updated>2017-05-12T12:06:31Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H2 surface is symmetric, the transition state must have r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance r&amp;lt;sub&amp;gt;AB&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;BC&amp;lt;/sub&amp;gt; are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt; estimated to be 0.9131A at this point of intersection.&lt;br /&gt;
By testing different initial conditions where r1 = r2 and p1 = p2 = 0, figure (X) shows the actual value of rts is determined to be 0.908 A&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620562</id>
		<title>MRD:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:YLS15&amp;diff=620562"/>
		<updated>2017-05-12T12:05:50Z</updated>

		<summary type="html">&lt;p&gt;Yls15: Created page with &amp;quot;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==  ===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, exp...&amp;quot;&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Exercise 1: H + H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; system ==&lt;br /&gt;
&lt;br /&gt;
===What value does the total gradient of the potential energy surface have at a minimum and at a transition structure? Briefly, explain how minima and transition structures can be distinguished using the curvature of the potential energy surface.===&lt;br /&gt;
&lt;br /&gt;
The total gradient of the potential energy surface is 0 both at the transition state and the minima. However, these can be distinguished using the value of the second derivatives.&lt;br /&gt;
The second derivative of the minima would be greater than zero as the minima is the lowest value on the potential energy surface.&lt;br /&gt;
The second derivative of the transition structure of the transition state would be less than zero. It would appear as a characteristic ‘saddle point’ on the potential energy surface.&lt;br /&gt;
&lt;br /&gt;
===Report your best estimate of the transition state position (r&amp;lt;sub&amp;gt;ts&amp;lt;/sub&amp;gt;) and explain your reasoning illustrating it with an “Internuclear Distances vs Time” screenshot for a relevant trajectory.===&lt;br /&gt;
&lt;br /&gt;
Since the H+H2 surface is symmetric, the transition state must have r1 = r2. Figure (x) shows as the time goes the 0.378 time units, the internuclear distance rAB and rBC are the same (r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). The value of the rts estimated to be 0.9131A at this point of intersection.&lt;br /&gt;
By testing different initial conditions where r1 = r2 and p1 = p2 = 0, figure (X) shows the actual value of rts is determined to be 0.908 A&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=544224</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=544224"/>
		<updated>2016-02-26T15:41:16Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen so the electron density is pulled toward the Nitrogen atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
==== Comparison with Literature Values ====&lt;br /&gt;
&lt;br /&gt;
The literature values of bond length and bond angles is taken from the [[http://cccbdb.nist.gov/exp2x.asp| NIST Computational Chemistry Comparison and Benchmark DataBase]].&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Comparison of Literature values and Calculated values&lt;br /&gt;
! Property !! Literature Value !! Calculated value !! Difference from the Literature value !! % Difference compared to the Literature value&lt;br /&gt;
|-&lt;br /&gt;
| H-N-H Bond Angle || 106.6700° || 105.7412° || -0.9288° || -0.87%&lt;br /&gt;
|-&lt;br /&gt;
| H-N Bond Length || 1.0124Å || 1.0180Å || +0.0056Å || +0.55%&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The calculated bond angle and bond length is very close to the literature value. The reason why the values does not match completely is because the basis set is &#039;&#039;&#039;6-31G(d,p)&#039;&#039;&#039; which only has medium accuracy. This basis set was used so the calculation is quick. For more accurate results, a basis set with higher accuracy should be used however the time taken to complete the calculation would be longer.&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The charge on the two Nitrogen atom is 0. The electrons are distributed evenly since as the two atoms have the same electronegativity as they are the same so there is no net dipole moment.&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The charge on the two Hydrogen atom is 0. The electrons are distributed evenly since as the two atoms have the same electronegativity as they are the same so there is no net dipole moment.&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen so the electron density is pulled toward the Carbon atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
Molecular orbitals 3, 4 and 5 are degenerate.&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 1&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 1s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This molecular orbital is very deep in energy.]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_2.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 2&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_3.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 3&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_4.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 4&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_5.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 5&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen. This is the highest occupied energy level (HOMO)]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_6.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 6&#039;&#039;&#039;-This is the unoccupied σ̈* anti-bonding molecular orbital form by destructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This is the lowest unoccupied molecular orbital (LUMO)]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=544188</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=544188"/>
		<updated>2016-02-26T15:35:37Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Comparison with literature values */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
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&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen so the electron density is pulled toward the Nitrogen atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
==== Comparison with literature values ====&lt;br /&gt;
&lt;br /&gt;
The literature values of bond length and bond angles is taken from the [[http://cccbdb.nist.gov/exp2x.asp| NIST Computational Chemistry Comparison and Benchmark DataBase]].&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Comparison of Literature values and Calculated values&lt;br /&gt;
! Property !! Literature Value !! Calculated value !! Difference from the Literature value !! % Difference compared to the Literature value&lt;br /&gt;
|-&lt;br /&gt;
| H-N-H Bond Angle || 106.6700° || 105.7412° || -0.9288° || -0.87%&lt;br /&gt;
|-&lt;br /&gt;
| H-N Bond Length || 1.0124Å || 1.0180Å || +0.0056Å || +0.55%&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The calculated bond angle and bond length is very close to the literature value. The reason why the values does not match completely is because the basis set is &#039;&#039;&#039;6-31G(d,p)&#039;&#039;&#039; which only has medium accuracy. This basis set was used so the calculation is quick. For more accurate results, a basis set with higher accuracy should be used however the time taken to complete the calculation would be longer.&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The charge on the two Nitrogen atom is 0. The electrons are distributed evenly since as the two atoms have the same electronegativity as they are the same so there is no net dipole moment.&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The charge on the two Hydrogen atom is 0. The electrons are distributed evenly since as the two atoms have the same electronegativity as they are the same so there is no net dipole moment.&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen so the electron density is pulled toward the Carbon atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
Molecular orbitals 3, 4 and 5 are degenerate.&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 1&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 1s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This molecular orbital is very deep in energy.]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_2.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 2&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_3.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 3&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_4.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 4&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_5.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 5&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen. This is the highest occupied energy level (HOMO)]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_6.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 6&#039;&#039;&#039;-This is the unoccupied σ̈* anti-bonding molecular orbital form by destructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This is the lowest unoccupied molecular orbital (LUMO)]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=544114</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=544114"/>
		<updated>2016-02-26T15:23:37Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Comparison with literature values */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen so the electron density is pulled toward the Nitrogen atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
==== Comparison with literature values ====&lt;br /&gt;
&lt;br /&gt;
The literature values of bond length and bond angles is taken from the [[http://cccbdb.nist.gov/exp2x.asp| NIST Computational Chemistry Comparison and Benchmark DataBase]].&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Comparison of Literature values and Calculated values&lt;br /&gt;
! Property !! Literature Value !! Calculated value !! Difference from the Literature value&lt;br /&gt;
|-&lt;br /&gt;
| H-N-H Bond Angle || 106.6700° || 105.7412° || -0.9288°&lt;br /&gt;
|-&lt;br /&gt;
| H-N Bond Length || 1.0124Å || 1.0180Å || +0.0056Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The charge on the two Nitrogen atom is 0. The electrons are distributed evenly since as the two atoms have the same electronegativity as they are the same so there is no net dipole moment.&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The charge on the two Hydrogen atom is 0. The electrons are distributed evenly since as the two atoms have the same electronegativity as they are the same so there is no net dipole moment.&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen so the electron density is pulled toward the Carbon atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
Molecular orbitals 3, 4 and 5 are degenerate.&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 1&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 1s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This molecular orbital is very deep in energy.]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_2.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 2&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_3.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 3&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_4.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 4&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_5.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 5&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen. This is the highest occupied energy level (HOMO)]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_6.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 6&#039;&#039;&#039;-This is the unoccupied σ̈* anti-bonding molecular orbital form by destructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This is the lowest unoccupied molecular orbital (LUMO)]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=544076</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=544076"/>
		<updated>2016-02-26T15:16:43Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen so the electron density is pulled toward the Nitrogen atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
==== Comparison with literature values ====&lt;br /&gt;
&lt;br /&gt;
The literature values of bond length and bond angles is taken from the 	NIST Computational Chemistry Comparison and Benchmark DataBase.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Comparison of Literature values and Calculated values&lt;br /&gt;
! Property !! Literature Value !! Calculated value&lt;br /&gt;
|-&lt;br /&gt;
| H-N-H Bond Angle || 106.6700° || 105.7412°&lt;br /&gt;
|-&lt;br /&gt;
| H-N Bond Length || 1.0124Å || 1.0180Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The charge on the two Nitrogen atom is 0. The electrons are distributed evenly since as the two atoms have the same electronegativity as they are the same so there is no net dipole moment.&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The charge on the two Hydrogen atom is 0. The electrons are distributed evenly since as the two atoms have the same electronegativity as they are the same so there is no net dipole moment.&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen so the electron density is pulled toward the Carbon atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
Molecular orbitals 3, 4 and 5 are degenerate.&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 1&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 1s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This molecular orbital is very deep in energy.]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_2.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 2&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_3.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 3&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_4.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 4&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_5.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 5&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen. This is the highest occupied energy level (HOMO)]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_6.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 6&#039;&#039;&#039;-This is the unoccupied σ̈* anti-bonding molecular orbital form by destructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This is the lowest unoccupied molecular orbital (LUMO)]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542704</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542704"/>
		<updated>2016-02-25T16:46:25Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Gaussian Calculation Summary */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen so the electron density is pulled toward the Nitrogen atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The charge on the two Nitrogen atom is 0. The electrons are distributed evenly since as the two atoms have the same electronegativity as they are the same so there is no net dipole moment.&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The charge on the two Hydrogen atom is 0. The electrons are distributed evenly since as the two atoms have the same electronegativity as they are the same so there is no net dipole moment.&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen so the electron density is pulled toward the Carbon atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
Molecular orbitals 3, 4 and 5 are degenerate.&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 1&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 1s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This molecular orbital is very deep in energy.]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_2.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 2&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_3.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 3&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_4.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 4&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_5.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 5&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen. This is the highest occupied energy level (HOMO)]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_6.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 6&#039;&#039;&#039;-This is the unoccupied σ̈* anti-bonding molecular orbital form by destructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This is the lowest unoccupied molecular orbital (LUMO)]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542701</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542701"/>
		<updated>2016-02-25T16:46:05Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Nitrogen, N2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen so the electron density is pulled toward the Nitrogen atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The charge on the two Nitrogen atom is 0. The electrons are distributed evenly since as the two atoms have the same electronegativity as they are the same so there is no net dipole moment.&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen so the electron density is pulled toward the Carbon atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
Molecular orbitals 3, 4 and 5 are degenerate.&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 1&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 1s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This molecular orbital is very deep in energy.]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_2.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 2&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_3.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 3&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_4.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 4&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_5.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 5&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen. This is the highest occupied energy level (HOMO)]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_6.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 6&#039;&#039;&#039;-This is the unoccupied σ̈* anti-bonding molecular orbital form by destructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This is the lowest unoccupied molecular orbital (LUMO)]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542665</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542665"/>
		<updated>2016-02-25T16:39:53Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Charge Distribution */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen so the electron density is pulled toward the Nitrogen atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen so the electron density is pulled toward the Carbon atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
Molecular orbitals 3, 4 and 5 are degenerate.&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 1&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 1s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This molecular orbital is very deep in energy.]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_2.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 2&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_3.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 3&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_4.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 4&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_5.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 5&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen. This is the highest occupied energy level (HOMO)]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_6.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 6&#039;&#039;&#039;-This is the unoccupied σ̈* anti-bonding molecular orbital form by destructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This is the lowest unoccupied molecular orbital (LUMO)]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542661</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542661"/>
		<updated>2016-02-25T16:39:29Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Charge Distribution */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen so the electron density is pulled toward the Nitrogen atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen so the electron density is pulled toward the carbon atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
&lt;br /&gt;
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Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
Molecular orbitals 3, 4 and 5 are degenerate.&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 1&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 1s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This molecular orbital is very deep in energy.]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_2.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 2&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_3.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 3&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_4.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 4&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_5.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 5&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen. This is the highest occupied energy level (HOMO)]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_6.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 6&#039;&#039;&#039;-This is the unoccupied σ̈* anti-bonding molecular orbital form by destructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This is the lowest unoccupied molecular orbital (LUMO)]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542657</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542657"/>
		<updated>2016-02-25T16:39:07Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Charge Distribution */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen so the electron density is pulled toward the carbon atom resulting in the negative charge.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
Molecular orbitals 3, 4 and 5 are degenerate.&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 1&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 1s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This molecular orbital is very deep in energy.]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_2.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 2&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_3.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 3&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_4.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 4&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_5.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 5&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen. This is the highest occupied energy level (HOMO)]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_6.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 6&#039;&#039;&#039;-This is the unoccupied σ̈* anti-bonding molecular orbital form by destructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This is the lowest unoccupied molecular orbital (LUMO)]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542642</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542642"/>
		<updated>2016-02-25T16:37:58Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Molecular Orbital */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
Molecular orbitals 3, 4 and 5 are degenerate.&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 1&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 1s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This molecular orbital is very deep in energy.]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_2.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 2&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_3.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 3&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_4.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 4&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_5.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 5&#039;&#039;&#039;-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen. This is the highest occupied energy level (HOMO)]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_6.PNG|thumb|left|&#039;&#039;&#039;Molecular Orbital 6&#039;&#039;&#039;-This is the unoccupied σ̈* anti-bonding molecular orbital form by destructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This is the lowest unoccupied molecular orbital (LUMO)]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542628</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542628"/>
		<updated>2016-02-25T16:35:44Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Molecular Orbital */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
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&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
Molecular Orbital 3, 4 and 5 are degenerate.&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|Molecular Orbital 1-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 1s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This molecular orbital is very deep in energy.]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_2.PNG|thumb|left|Molecular Orbital 2-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_3.PNG|thumb|left|Molecular Orbital 3-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_4.PNG|thumb|left|Molecular Orbital 4-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_5.PNG|thumb|left|Molecular Orbital 5-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen. This is the highest occupied energy level (HOMO)]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_6.PNG|thumb|left|Molecular Orbital 6-This is the unoccupied σ̈* anti-bonding molecular orbital form by destructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This is the lowest unoccupied molecular orbital (LUMO)]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542622</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542622"/>
		<updated>2016-02-25T16:33:51Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Molecular Orbital */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|Molecular Orbital 1-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 1s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This molecular orbital is very deep in energy.]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_2.PNG|thumb|left|Molecular Orbital 2-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_3.PNG|thumb|left|Molecular Orbital 3-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_4.PNG|thumb|left|Molecular Orbital 4-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_5.PNG|thumb|left|Molecular Orbital 5-This is the occupied σ bonding molecular orbital formed by constructive overlap of the 2s atomic orbital of Carbon and the 2p atomic orbital of Hydrogen. This is the highest occupied energy level (HOMO)]]&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_6.PNG|thumb|left|Molecular Orbital 6-This is the unoccupied σ̈* anti-bonding molecular orbital form by destructive overlap of the 2s atomic orbital of Carbon and the 1s atomic orbital of Hydrogen. This is the lowest unoccupied molecular orbital (LUMO)]]&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542482</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542482"/>
		<updated>2016-02-25T16:15:59Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Charge Distribution */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
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&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.233&lt;br /&gt;
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Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:Yls_15_MO_1.PNG|thumb|left|Molecular Orbital 1]][[File:Yls_15_MO_2.PNG|thumb|left|Molecular Orbital 2]][[File:Yls_15_MO_3.PNG|thumb|right|Molecular Orbital 3]][[File:Yls_15_MO_4.PNG|thumb|left|Molecular Orbital 4]][[File:Yls_15_MO_5.PNG|thumb|left|Molecular Orbital 5]][[File:Yls_15_MO_6.PNG|thumb|left|Molecular Orbital 6]]&lt;br /&gt;
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1= 1s sigma bond&lt;br /&gt;
2= 2s sigma bond&lt;br /&gt;
3=s-p sigma bond&lt;br /&gt;
4=s-p sigma bond&lt;br /&gt;
5=s-p sigma bond&lt;br /&gt;
6= 2s sigma star bond&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542480</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542480"/>
		<updated>2016-02-25T16:15:49Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Molecular Orbital */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
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The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.233&lt;br /&gt;
&lt;br /&gt;
Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
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[[File:Yls_15_MO_1.PNG|thumb|left|Molecular Orbital 1]][[File:Yls_15_MO_2.PNG|thumb|left|Molecular Orbital 2]][[File:Yls_15_MO_3.PNG|thumb|right|Molecular Orbital 3]][[File:Yls_15_MO_4.PNG|thumb|left|Molecular Orbital 4]][[File:Yls_15_MO_5.PNG|thumb|left|Molecular Orbital 5]][[File:Yls_15_MO_6.PNG|thumb|left|Molecular Orbital 6]]&lt;br /&gt;
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1= 1s sigma bond&lt;br /&gt;
2= 2s sigma bond&lt;br /&gt;
3=s-p sigma bond&lt;br /&gt;
4=s-p sigma bond&lt;br /&gt;
5=s-p sigma bond&lt;br /&gt;
6= 2s sigma star bond&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542458</id>
		<title>Rep:Mod:YLS15</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:YLS15&amp;diff=542458"/>
		<updated>2016-02-25T16:13:12Z</updated>

		<summary type="html">&lt;p&gt;Yls15: /* Methane, CH4 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Ammonia, NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -56.55776873 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000485 a.u.&lt;br /&gt;
* The point group of your molecule: C&amp;lt;sub&amp;gt;3v&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-N-H bond angle:105.7412°&lt;br /&gt;
* H-N bond length: 1.018Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_NH3_OPTIMISATION.LOG| here]]&lt;br /&gt;
&amp;lt;pre&amp;gt; Item                     Value      Threshold  Converged?&lt;br /&gt;
&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
 Predicted change in Energy=-5.986284D-10&lt;br /&gt;
&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
&lt;br /&gt;
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !&lt;br /&gt;
&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;NH3 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_NH3_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Vibration_Frequencies.PNG]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule [[Media:YLS15_vibrations_1.gif| Mode 1]][[Media:YLS15_vibrations_2.gif| Mode 2]][[Media:YLS15_vibrations_3.gif| Mode 3]][[Media:YLS15_vibrations_4.gif| Mode 4]][[Media:YLS15_vibrations_5.gif| Mode 5]][[Media:YLS15_vibrations_6.gif| Mode 6]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
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&#039;&#039;&#039;How many modes do you expect from the 3N-6 rule?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
6 Vibration modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are degenerate (ie have the same energy)?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are degenerate. Also modes 5 and 6 are degenerate.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Which modes are &amp;quot;bending&amp;quot; vibrations and which are &amp;quot;bond stretch&amp;quot; vibrations?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 2 and 3 are &amp;quot;bending&amp;quot; vibrations, mode 4 is symmetrical stretching, modes 5 and 6 are asymmetrical stretching.&lt;br /&gt;
 &lt;br /&gt;
&#039;&#039;&#039;Which mode is highly symmetric?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1 and 4 is highly symmetrical.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;One mode is known as the &amp;quot;umbrella&amp;quot; mode, which one is this?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Mode 1&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;How many bands would you expect to see in an experimental spectrum of gaseous ammonia?&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
2 Bands at 1089.54 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and 1693.95 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
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The charge on the Nitrogen atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Nitrogen is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_Charge_Distribution.PNG|thumb|left|Charge Distribution of a NH3 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.375&lt;br /&gt;
&lt;br /&gt;
Charge on the Nitrogen atom: -1.125&lt;br /&gt;
&lt;br /&gt;
== Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Nitrogen, N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -109.52412868 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000217 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* N≡N bond angle: 180°&lt;br /&gt;
* N≡N bond length: 1.1055Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_N2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000001     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000002     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-4.428714D-12&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 2457.34 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Hydrogen, H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -1.17853936 a.u.&lt;br /&gt;
* RMS Gradient: 0.00000017 a.u.&lt;br /&gt;
* The point group of your molecule: D∞h&lt;br /&gt;
* H-H bond angle: 180°&lt;br /&gt;
* H-H bond length: 0.7428Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_H2_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000000     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000000     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000001     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-1.164080D-13&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One vibration mode occurs at 4465.68 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Reaction Energy of the Haber-Bosch process ==&lt;br /&gt;
&lt;br /&gt;
* E(NH3)= -56.55776873 a.u.&lt;br /&gt;
* 2*E(NH3)= -113.11553746 a.u.&lt;br /&gt;
* E(N2)= -109.52412868 a.u.&lt;br /&gt;
* E(H2)= -1.17853936 a.u.&lt;br /&gt;
* 3*E(H2)= -3.53561808 a.u.&lt;br /&gt;
* ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.0557907 a.u. = -146.4784828 kJ moɭ &amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ΔE is a negative value which indicated that the gaseous product is more stable.&lt;br /&gt;
&lt;br /&gt;
== Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; ==&lt;br /&gt;
&lt;br /&gt;
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==== Gaussian Calculation Summary ====&lt;br /&gt;
* Molecule Name: Methane, CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;&lt;br /&gt;
* Calculation Method: RB3LYP&lt;br /&gt;
* Basis set:6-31G(d,p)&lt;br /&gt;
* Final energy E(RB3LYP): -40.52401404 a.u.&lt;br /&gt;
* RMS Gradient: 0.00003263 a.u.&lt;br /&gt;
* The point group of your molecule: T&amp;lt;sub&amp;gt;d&amp;lt;/sub&amp;gt;&lt;br /&gt;
* H-C-H bond angle:109.4712°&lt;br /&gt;
* C-H bond length: 1.092Å&lt;br /&gt;
&lt;br /&gt;
The optimisation file of CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; is linked [[Media:YLS15_CH4_OPTIMISED.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;pre&amp;gt; Item                     Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000063     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000034     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000179     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000095     0.001200     YES&lt;br /&gt;
 Predicted change in Energy=-2.256106D-08&lt;br /&gt;
 Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
                           ----------------------------&lt;br /&gt;
                           !   Optimized Parameters   !&lt;br /&gt;
                           ! (Angstroms and Degrees)  !&lt;br /&gt;
 --------------------------                            --------------------------&lt;br /&gt;
 ! Name  Definition              Value          Derivative Info.                !&lt;br /&gt;
 --------------------------------------------------------------------------------&lt;br /&gt;
 ! R1    R(1,2)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R2    R(1,3)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R3    R(1,4)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! R4    R(1,5)                  1.092          -DE/DX =   -0.0001              !&lt;br /&gt;
 ! A1    A(2,1,3)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A2    A(2,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A3    A(2,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A4    A(3,1,4)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A5    A(3,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! A6    A(4,1,5)              109.4712         -DE/DX =    0.0                 !&lt;br /&gt;
 ! D1    D(2,1,4,3)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D2    D(2,1,5,3)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D3    D(2,1,5,4)            120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 ! D4    D(3,1,5,4)           -120.0            -DE/DX =    0.0                 !&lt;br /&gt;
 --------------------------------------------------------------------------------&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;CH4 Molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;400&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;YLS15_CH4_OPTIMISED.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====Vibration Modes====&lt;br /&gt;
&lt;br /&gt;
[[File:CH4_Vibrations.PNG]]&lt;br /&gt;
&lt;br /&gt;
Using the 3N-6 rule, the methane molecule is expected to have 9 vibrational modes.&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;The animations of the different vibrations modes of the CH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; molecule &#039;&#039;&#039;[[Media:YLS15_CH4_Vibration_1.gif| Mode 1]][[Media:YLS15_CH4_Vibration_2.gif| Mode 2]][[Media:YLS15_CH4_Vibration_3.gif| Mode 3]][[Media:YLS15_CH4_Vibration_4.gif| Mode 4]][[Media:YLS15_CH4_Vibration_5.gif| Mode 5]][[Media:YLS15_CH4_Vibration_6.gif| Mode 6]][[Media:YLS15_CH4_Vibration_7.gif| Mode 7]][[Media:YLS15_CH4_Vibration_8.gif| Mode 8]][[Media:YLS15_CH4_Vibration_9.gif| Mode 9]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Modes 1, 2 and 3 are degenerate. Modes 4 and 5 are degenerate. Modes 7, 8 and 9 are also degenerate.&lt;br /&gt;
&lt;br /&gt;
̈Modes 1, 2, 3, 4 and 5 are &amp;quot;bending vibrations. Mode 6 is symmetrical stretching. Modes 7 and 8 are asymmetrical stretching.&lt;br /&gt;
&lt;br /&gt;
====Charge Distribution====&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The charge on the Carbon atom is expected to be negative and the charge on the Hydrogen atom is expected to be positive as Carbon is more electronegative than Hydrogen.&lt;br /&gt;
&lt;br /&gt;
[[File:YLS15_CH4_CHARGE_DISTRIBUTION.PNG|thumb|left|Charge Distribution of a CH4 molecule]]&lt;br /&gt;
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Charge on the Hydrogen atom: +0.233&lt;br /&gt;
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Charge on the Carbon atom: -0.930&lt;br /&gt;
&lt;br /&gt;
==== Molecular Orbital ====&lt;br /&gt;
&lt;br /&gt;
Yls_15_MO_6.PNG&lt;br /&gt;
&lt;br /&gt;
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1= 1s sigma bond&lt;br /&gt;
2= 2s sigma bond&lt;br /&gt;
3=s-p sigma bond&lt;br /&gt;
4=s-p sigma bond&lt;br /&gt;
5=s-p sigma bond&lt;br /&gt;
6= 2s sigma star bond&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls_15_MO_6.PNG&amp;diff=542453</id>
		<title>File:Yls 15 MO 6.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls_15_MO_6.PNG&amp;diff=542453"/>
		<updated>2016-02-25T16:12:48Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls_15_MO_5.PNG&amp;diff=542448</id>
		<title>File:Yls 15 MO 5.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls_15_MO_5.PNG&amp;diff=542448"/>
		<updated>2016-02-25T16:12:29Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls_15_MO_4.PNG&amp;diff=542445</id>
		<title>File:Yls 15 MO 4.PNG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Yls_15_MO_4.PNG&amp;diff=542445"/>
		<updated>2016-02-25T16:12:19Z</updated>

		<summary type="html">&lt;p&gt;Yls15: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Yls15</name></author>
	</entry>
</feed>