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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811628</id>
		<title>MRD:cid-01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811628"/>
		<updated>2020-05-22T21:43:40Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Question 1 ==&lt;br /&gt;
===Mathematical definition of transition state===&lt;br /&gt;
When modelling a potential energy surface of a chemical reaction, the transition state is a point on the minimum energy reaction pathway with maximum potential energy. Firstly, it is in the minimum energy pathway,so it is a minimum perpendicular to the reaction pathway. then, maximum potential energy appears at this point, means it is maximum alone the reaction pathway&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;. This sort of point are mathematically defined as a saddle point of a surface. &lt;br /&gt;
===Identification of transition state===&lt;br /&gt;
As the transition state can be represent by a saddle point, it is possible to apply mathematical methods&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt; of identifying stationary points to determine whether a stationary point represent the stationary point or not. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Mathematical method of identifying stationary points of a surface&lt;br /&gt;
! type of stationary points !! identification methond &lt;br /&gt;
|-&lt;br /&gt;
| local maximum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;lt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| local minimum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;gt; 0 &amp;lt;/math&amp;gt; &lt;br /&gt;
|-&lt;br /&gt;
| saddle point || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2}\frac {\partial^2 }{\partial y^2}-\frac {\partial^2 }{\partial xy}\frac {\partial^2 }{\partial yx} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
For a potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). In order to identify if a point with certain reaction coordinates represent the transition state or not, we can substitute the reaction coordinates into the function &amp;lt;math&amp;gt;\frac {\partial^2V }{\partial r_1^2}\frac {\partial^2V }{\partial r_2^2}-\frac {\partial^2V }{\partial r_1r_2y}\frac {\partial^2V }{\partial r_2r_1}&amp;lt;/math&amp;gt;. If the result is negative, it is the saddle point if the potential surface, and can represent the transition state. &lt;br /&gt;
==Question 2==&lt;br /&gt;
===Transition state position estimation===&lt;br /&gt;
For the reaction of a hydrogen atom collides with a hydrogen molecule at 180 degree to form a new hydrogen molecule and release an other hydrogen atom, consider there are only two degrees of freedom involved in the function of potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;), where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is the distance between the free atom and one end of the molecule, and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is the distance between the two H atoms originally in the hydrogen molecule. The system is symmetric, so r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are equal at the transition state. Secondly, for a stationary point, we have &amp;lt;math&amp;gt;\frac {\partial V }{\partial v_1}=\frac {\partial V}{\partial v_2}=0&amp;lt;/math&amp;gt;. The first derivative of potential is force. Therefore, in order to find the best estimation of the transition state. We need to run estimations with different r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, until we find the force alone the direction of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are both 0. The modelling starts from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=230pm(the initial distance between the free H atom and hydrogen molecule), and the best estimation is r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=90.775pm. &lt;br /&gt;
&lt;br /&gt;
==Question 3==&lt;br /&gt;
===Reaction trajectories calculation===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|-&lt;br /&gt;
|[[File:Dym-01554120.png|250px]]||[[File:MEP1-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
The picture on the left hand side shows the reaction trajectory calculated under dynamic type, it includes the vibrational level of the molecules after they enter the product side. the picture on the right hand side is the reaction trajectory under &amp;lt;i&amp;gt;mep&amp;lt;/i&amp;gt; type calculation, and the vibrational levels are not included within this calculation. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|-&lt;br /&gt;
|[[File:MT-c1-01554120.png|250px]]||[[File:flatmomentum-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
The picture on the left is the momenta-time graph under dynamic type calculation, the momenta of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are included in this calculation. The picture on the right is momenta-time graph obtained under &amp;lt;i&amp;gt;mep&amp;lt;/i&amp;gt; type calculation, which ignored the momenta of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
==Question 4==&lt;br /&gt;
in this section A represent the original free H atom, B is the H atom in hydrogen molecule that collide with A, and C the H atom leaving the molecule after collision. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280|| Yes||The reactants successfully pass through the transition state and reaches the product. ||[[File:Animation1-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077|| No||The reactants cannot pass through the transition state, and bounce back to the reactants.  ||[[File:Animation2-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977|| Yes|| The reactants successfully pass through the transition state and reaches the product.||[[File:Animation3-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277|| No|| The reactants successfully pass through the transition state, however, they bounce back in to the reactants with a higher level of vibrational state.||[[File:Animation4-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477|| Yes||The reactants successfully pass through the transition state, then it bounce back once and enter the product side once again. The products formed are in a higher level vibrational state. ||[[File:Animation5-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
According to the table, momenta of molecules become more negative from the top to the bottom. It will be not appropriate to conclude a relation between reactivities and momenta(which represent the initial speeds of molecules). However, the total energies become less negative with more negative momenta. So we can conclude that energy can not solely determine the reactivity of an reaction. &lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;br /&gt;
&amp;lt;p&amp;gt;1. Dill KA, Bromberg S. Chapter 19, Chemical Kinetics &amp;amp; Transition States. In:&amp;lt;i&amp;gt;Molecular Driving Force: Statistical Thermodynamics in Biology, Chemistry, Physics and Nanoscience&amp;lt;/i&amp;gt;.2nd ed. United States of America: Garland Science, Taylor &amp;amp; Francis Group, LLC; 2010. p.364-365. &amp;lt;/p&amp;gt;&lt;br /&gt;
&amp;lt;p&amp;gt;2. Steiner E. Chapter 9, Functions of Several Variables, In: &amp;lt;i&amp;gt;The Chemistry Maths Book&amp;lt;/i&amp;gt;. 2nd ed. United States: Oxford University Press; 2008. p.253-255.&amp;lt;/p&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811563</id>
		<title>MRD:cid-01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811563"/>
		<updated>2020-05-22T21:26:34Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Question 1 ==&lt;br /&gt;
===Mathematical definition of transition state===&lt;br /&gt;
When modelling a potential energy surface of a chemical reaction, the transition state is a point on the minimum energy reaction pathway with maximum potential energy. Firstly, it is in the minimum energy pathway,so it is a minimum perpendicular to the reaction pathway. then, maximum potential energy appears at this point, means it is maximum alone the reaction pathway&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;. This sort of point are mathematically defined as a saddle point of a surface. &lt;br /&gt;
===Identification of transition state===&lt;br /&gt;
As the transition state can be represent by a saddle point, it is possible to apply mathematical methods&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt; of identifying stationary points to determine whether a stationary point represent the stationary point or not. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Mathematical method of identifying stationary points of a surface&lt;br /&gt;
! type of stationary points !! identification methond &lt;br /&gt;
|-&lt;br /&gt;
| local maximum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;lt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| local minimum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;gt; 0 &amp;lt;/math&amp;gt; &lt;br /&gt;
|-&lt;br /&gt;
| saddle point || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2}\frac {\partial^2 }{\partial y^2}-\frac {\partial^2 }{\partial xy}\frac {\partial^2 }{\partial yx} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
For a potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). In order to identify if a point with certain reaction coordinates represent the transition state or not, we can substitute the reaction coordinates into the function &amp;lt;math&amp;gt;\frac {\partial^2V }{\partial r_1^2}\frac {\partial^2V }{\partial r_2^2}-\frac {\partial^2V }{\partial r_1r_2y}\frac {\partial^2V }{\partial r_2r_1}&amp;lt;/math&amp;gt;. If the result is negative, it is the saddle point if the potential surface, and can represent the transition state. &lt;br /&gt;
==Question 2==&lt;br /&gt;
===Transition state position estimation===&lt;br /&gt;
For the reaction of a hydrogen atom collides with a hydrogen molecule at 180 degree to form a new hydrogen molecule and release an other hydrogen atom, consider there are only two degrees of freedom involved in the function of potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;), where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is the distance between the free atom and one end of the molecule, and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is the distance between the two H atoms originally in the hydrogen molecule. The system is symmetric, so r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are equal at the transition state. Secondly, for a stationary point, we have &amp;lt;math&amp;gt;\frac {\partial V }{\partial v_1}=\frac {\partial V}{\partial v_2}=0&amp;lt;/math&amp;gt;. The first derivative of potential is force. Therefore, in order to find the best estimation of the transition state. We need to run estimations with different r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, until we find the force alone the direction of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are both 0. The modelling starts from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=230pm(the initial distance between the free H atom and hydrogen molecule), and the best estimation is r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=90.775pm. &lt;br /&gt;
&lt;br /&gt;
==Question 3==&lt;br /&gt;
===Reaction trajectories calculation===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|-&lt;br /&gt;
|[[File:Dym-01554120.png|250px]]||[[File:MEP1-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
The picture on the left hand side shows the reaction trajectory calculated under dynamic type, it includes the vibrational level of the molecules after they enter the product side. the picture on the right hand side is the reaction trajectory under &amp;lt;i&amp;gt;mep&amp;lt;/i&amp;gt; type calculation, and the vibrational levels are not included within this calculation. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|-&lt;br /&gt;
|[[File:MT-c1-01554120.png|250px]]||[[File:flatmomentum-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
The picture on the left is the momenta-time graph under dynamic type calculation, the momenta of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are included in this calculation. The picture on the right is momenta-time graph obtained under &amp;lt;i&amp;gt;mep&amp;lt;/i&amp;gt; type calculation, which ignored the momenta of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
==Question 4==&lt;br /&gt;
in this section A represent the original free H atom, B is the H atom in hydrogen molecule that collide with A, and C the H atom leaving the molecule after collision. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280|| Yes||The reactants successfully pass through the transition state and reaches the product. ||[[File:Animation1-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077|| No||The reactants cannot pass through the transition state, and bounce back to the reactants.  ||[[File:Animation2-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977|| Yes|| The reactants successfully pass through the transition state and reaches the product.||[[File:Animation3-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277|| No|| The reactants successfully pass through the transition state, however, they bounce back in to the reactants with a higher level of vibrational state.||[[File:Animation4-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477|| Yes||The reactants successfully pass through the transition state, then it bounce back once and enter the product side once again. The products formed are in a higher level vibrational state. ||[[File:Animation5-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;br /&gt;
&amp;lt;p&amp;gt;1. Dill KA, Bromberg S. Chapter 19, Chemical Kinetics &amp;amp; Transition States. In:&amp;lt;i&amp;gt;Molecular Driving Force: Statistical Thermodynamics in Biology, Chemistry, Physics and Nanoscience&amp;lt;/i&amp;gt;.2nd ed. United States of America: Garland Science, Taylor &amp;amp; Francis Group, LLC; 2010. p.364-365. &amp;lt;/p&amp;gt;&lt;br /&gt;
&amp;lt;p&amp;gt;2. Steiner E. Chapter 9, Functions of Several Variables, In: &amp;lt;i&amp;gt;The Chemistry Maths Book&amp;lt;/i&amp;gt;. 2nd ed. United States: Oxford University Press; 2008. p.253-255.&amp;lt;/p&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811458</id>
		<title>MRD:cid-01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811458"/>
		<updated>2020-05-22T20:59:51Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Question 1 ==&lt;br /&gt;
===Mathematical definition of transition state===&lt;br /&gt;
When modelling a potential energy surface of a chemical reaction, the transition state is a point on the minimum energy reaction pathway with maximum potential energy. Firstly, it is in the minimum energy pathway,so it is a minimum perpendicular to the reaction pathway. then, maximum potential energy appears at this point, means it is maximum alone the reaction pathway&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;. This sort of point are mathematically defined as a saddle point of a surface. &lt;br /&gt;
===Identification of transition state===&lt;br /&gt;
As the transition state can be represent by a saddle point, it is possible to apply mathematical methods&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt; of identifying stationary points to determine whether a stationary point represent the stationary point or not. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Mathematical method of identifying stationary points of a surface&lt;br /&gt;
! type of stationary points !! identification methond &lt;br /&gt;
|-&lt;br /&gt;
| local maximum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;lt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| local minimum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;gt; 0 &amp;lt;/math&amp;gt; &lt;br /&gt;
|-&lt;br /&gt;
| saddle point || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2}\frac {\partial^2 }{\partial y^2}-\frac {\partial^2 }{\partial xy}\frac {\partial^2 }{\partial yx} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
For a potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). In order to identify if a point with certain reaction coordinates represent the transition state or not, we can substitute the reaction coordinates into the function &amp;lt;math&amp;gt;\frac {\partial^2V }{\partial r_1^2}\frac {\partial^2V }{\partial r_2^2}-\frac {\partial^2V }{\partial r_1r_2y}\frac {\partial^2V }{\partial r_2r_1}&amp;lt;/math&amp;gt;. If the result is negative, it is the saddle point if the potential surface, and can represent the transition state. &lt;br /&gt;
==Question 2==&lt;br /&gt;
===Transition state position estimation===&lt;br /&gt;
For the reaction of a hydrogen atom collides with a hydrogen molecule at 180 degree to form a new hydrogen molecule and release an other hydrogen atom, consider there are only two degrees of freedom involved in the function of potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;), where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is the distance between the free atom and one end of the molecule, and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is the distance between the two H atoms originally in the hydrogen molecule. The system is symmetric, so r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are equal at the transition state. Secondly, for a stationary point, we have &amp;lt;math&amp;gt;\frac {\partial V }{\partial v_1}=\frac {\partial V}{\partial v_2}=0&amp;lt;/math&amp;gt;. The first derivative of potential is force. Therefore, in order to find the best estimation of the transition state. We need to run estimations with different r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, until we find the force alone the direction of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are both 0. The modelling starts from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=230pm(the initial distance between the free H atom and hydrogen molecule), and the best estimation is r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=90.775pm. &lt;br /&gt;
&lt;br /&gt;
==Question 3==&lt;br /&gt;
===Reaction trajectories calculation===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|-&lt;br /&gt;
|[[File:Dym-01554120.png|250px]]||[[File:MEP1-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
The picture on the left hand side shows the reaction trajectory calculated under dynamic type, it includes the vibrational level of the molecules after they enter the product side. the picture on the right hand side is the reaction trajectory under &amp;lt;i&amp;gt;mep&amp;lt;/i&amp;gt; type calculation, and the vibrational levels are not included within this calculation. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|-&lt;br /&gt;
|[[File:MT-c1-01554120.png|250px]]||[[File:flatmomentum-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
The picture on the left is the momenta-time graph under dynamic type calculation, the momenta of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are included in this calculation. The picture on the right is momenta-time graph obtained under &amp;lt;i&amp;gt;mep&amp;lt;/i&amp;gt; type calculation, which ignored the momenta of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
==Question 4==&lt;br /&gt;
in this section A represent the original free H atom, B is the H atom in hydrogen molecule that collide with A, and C the H atom leaving the molecule after collision. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280|| Yes||The reactants successfully pass through the transition state and reaches the product. ||[[File:Animation1-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077|| No||The reactants cannot pass through the transition state, and bounce back to the reactants.  ||[[File:Animation2-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977|| Yes|| The reactants successfully pass through the transition state and reaches the product.||[[File:Animation3-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277|| No|| The reactants successfully pass through the transition state, however, they bounce back in to the reactants with a higher level of vibrational state.||[[File:Animation4-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477|| Yes||The reactants successfully pass through the transition state, then it bounce back once and enter the product side once again. The products formed are in a higher level vibrational state. ||[[File:Animation5-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;br /&gt;
1. Molecular Driving force&lt;br /&gt;
2. Chemistry math book&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811440</id>
		<title>MRD:cid-01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811440"/>
		<updated>2020-05-22T20:53:07Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Question 1 ==&lt;br /&gt;
===Mathematical definition of transition state===&lt;br /&gt;
When modelling a potential energy surface of a chemical reaction, the transition state is a point on the minimum energy reaction pathway with maximum potential energy. Firstly, it is in the minimum energy pathway,so it is a minimum perpendicular to the reaction pathway. then, maximum potential energy appears at this point, means it is maximum alone the reaction pathway&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;. This sort of point are mathematically defined as a saddle point of a surface. &lt;br /&gt;
===Identification of transition state===&lt;br /&gt;
As the transition state can be represent by a saddle point, it is possible to apply mathematical methods&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt; of identifying stationary points to determine whether a stationary point represent the stationary point or not. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Mathematical method of identifying stationary points of a surface&lt;br /&gt;
! type of stationary points !! identification methond &lt;br /&gt;
|-&lt;br /&gt;
| local maximum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;lt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| local minimum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;gt; 0 &amp;lt;/math&amp;gt; &lt;br /&gt;
|-&lt;br /&gt;
| saddle point || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2}\frac {\partial^2 }{\partial y^2}-\frac {\partial^2 }{\partial xy}\frac {\partial^2 }{\partial yx} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
For a potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). In order to identify if a point with certain reaction coordinates represent the transition state or not, we can substitute the reaction coordinates into the function &amp;lt;math&amp;gt;\frac {\partial^2V }{\partial r_1^2}\frac {\partial^2V }{\partial r_2^2}-\frac {\partial^2V }{\partial r_1r_2y}\frac {\partial^2V }{\partial r_2r_1}&amp;lt;/math&amp;gt;. If the result is negative, it is the saddle point if the potential surface, and can represent the transition state. &lt;br /&gt;
==Question 2==&lt;br /&gt;
===Transition state position estimation===&lt;br /&gt;
For the reaction of a hydrogen atom collides with a hydrogen molecule at 180 degree to form a new hydrogen molecule and release an other hydrogen atom, consider there are only two degrees of freedom involved in the function of potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;), where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is the distance between the free atom and one end of the molecule, and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is the distance between the two H atoms originally in the hydrogen molecule. The system is symmetric, so r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are equal at the transition state. Secondly, for a stationary point, we have &amp;lt;math&amp;gt;\frac {\partial V }{\partial v_1}=\frac {\partial V}{\partial v_2}=0&amp;lt;/math&amp;gt;. The first derivative of potential is force. Therefore, in order to find the best estimation of the transition state. We need to run estimations with different r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, until we find the force alone the direction of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are both 0. The modelling starts from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=230pm(the initial distance between the free H atom and hydrogen molecule), and the best estimation is r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=90.775pm. &lt;br /&gt;
&lt;br /&gt;
==Question 3==&lt;br /&gt;
===Reaction trajectories calculation===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|-&lt;br /&gt;
|[[File:Dym-01554120.png|250px]]||[[File:MEP1-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|-&lt;br /&gt;
|[[File:MT-c1-01554120.png|250px]]||[[File:flatmomentum-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
==Question 4==&lt;br /&gt;
in this section A represent the original free H atom, B is the H atom in hydrogen molecule that collide with A, and C the H atom leaving the molecule after collision. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280|| Yes||The reactants successfully pass through the transition state and reaches the product. ||[[File:Animation1-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077|| No||The reactants cannot pass through the transition state, and bounce back to the reactants.  ||[[File:Animation2-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977|| Yes|| The reactants successfully pass through the transition state and reaches the product.||[[File:Animation3-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277|| No|| The reactants successfully pass through the transition state, however, they bounce back in to the reactants with a higher level of vibrational state.||[[File:Animation4-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477|| Yes||The reactants successfully pass through the transition state, then it bounce back once and enter the product side once again. The products formed are in a higher level vibrational state. ||[[File:Animation5-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;br /&gt;
1. Molecular Driving force&lt;br /&gt;
2. Chemistry math book&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811435</id>
		<title>MRD:cid-01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811435"/>
		<updated>2020-05-22T20:52:01Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Question 1 ==&lt;br /&gt;
===Mathematical definition of transition state===&lt;br /&gt;
When modelling a potential energy surface of a chemical reaction, the transition state is a point on the minimum energy reaction pathway with maximum potential energy. Firstly, it is in the minimum energy pathway,so it is a minimum perpendicular to the reaction pathway. then, maximum potential energy appears at this point, means it is maximum alone the reaction pathway&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;. This sort of point are mathematically defined as a saddle point of a surface. &lt;br /&gt;
===Identification of transition state===&lt;br /&gt;
As the transition state can be represent by a saddle point, it is possible to apply mathematical methods&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt; of identifying stationary points to determine whether a stationary point represent the stationary point or not. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Mathematical method of identifying stationary points of a surface&lt;br /&gt;
! type of stationary points !! identification methond &lt;br /&gt;
|-&lt;br /&gt;
| local maximum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;lt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| local minimum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;gt; 0 &amp;lt;/math&amp;gt; &lt;br /&gt;
|-&lt;br /&gt;
| saddle point || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2}\frac {\partial^2 }{\partial y^2}-\frac {\partial^2 }{\partial xy}\frac {\partial^2 }{\partial yx} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
For a potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). In order to identify if a point with certain reaction coordinates represent the transition state or not, we can substitute the reaction coordinates into the function &amp;lt;math&amp;gt;\frac {\partial^2V }{\partial r_1^2}\frac {\partial^2V }{\partial r_2^2}-\frac {\partial^2V }{\partial r_1r_2y}\frac {\partial^2V }{\partial r_2r_1}&amp;lt;/math&amp;gt;. If the result is negative, it is the saddle point if the potential surface, and can represent the transition state. &lt;br /&gt;
==Question 2==&lt;br /&gt;
===Transition state position estimation===&lt;br /&gt;
For the reaction of a hydrogen atom collides with a hydrogen molecule at 180 degree to form a new hydrogen molecule and release an other hydrogen atom, consider there are only two degrees of freedom involved in the function of potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;), where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is the distance between the free atom and one end of the molecule, and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is the distance between the two H atoms originally in the hydrogen molecule. The system is symmetric, so r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are equal at the transition state. Secondly, for a stationary point, we have &amp;lt;math&amp;gt;\frac {\partial V }{\partial v_1}=\frac {\partial V}{\partial v_2}=0&amp;lt;/math&amp;gt;. The first derivative of potential is force. Therefore, in order to find the best estimation of the transition state. We need to run estimations with different r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, until we find the force alone the direction of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are both 0. The modelling starts from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=230pm(the initial distance between the free H atom and hydrogen molecule), and the best estimation is r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=90.775pm. &lt;br /&gt;
&lt;br /&gt;
==Question 3==&lt;br /&gt;
===Reaction trajectories calculation===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
|-&lt;br /&gt;
|[[File:MT-c1-01554120.png|250px]]||[[File:flatmomentum-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
==Question 4==&lt;br /&gt;
in this section A represent the original free H atom, B is the H atom in hydrogen molecule that collide with A, and C the H atom leaving the molecule after collision. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280|| Yes||The reactants successfully pass through the transition state and reaches the product. ||[[File:Animation1-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077|| No||The reactants cannot pass through the transition state, and bounce back to the reactants.  ||[[File:Animation2-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977|| Yes|| The reactants successfully pass through the transition state and reaches the product.||[[File:Animation3-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277|| No|| The reactants successfully pass through the transition state, however, they bounce back in to the reactants with a higher level of vibrational state.||[[File:Animation4-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477|| Yes||The reactants successfully pass through the transition state, then it bounce back once and enter the product side once again. The products formed are in a higher level vibrational state. ||[[File:Animation5-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;br /&gt;
1. Molecular Driving force&lt;br /&gt;
2. Chemistry math book&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:MT-c1-01554120.png&amp;diff=811417</id>
		<title>File:MT-c1-01554120.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:MT-c1-01554120.png&amp;diff=811417"/>
		<updated>2020-05-22T20:43:25Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Flatmomentum-01554120.png&amp;diff=811414</id>
		<title>File:Flatmomentum-01554120.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Flatmomentum-01554120.png&amp;diff=811414"/>
		<updated>2020-05-22T20:42:23Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Dym-01554120.png&amp;diff=811391</id>
		<title>File:Dym-01554120.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Dym-01554120.png&amp;diff=811391"/>
		<updated>2020-05-22T20:33:20Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:MEP1-01554120.png&amp;diff=811390</id>
		<title>File:MEP1-01554120.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:MEP1-01554120.png&amp;diff=811390"/>
		<updated>2020-05-22T20:32:41Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811364</id>
		<title>MRD:cid-01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811364"/>
		<updated>2020-05-22T20:22:28Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Question 1 ==&lt;br /&gt;
===Mathematical definition of transition state===&lt;br /&gt;
When modelling a potential energy surface of a chemical reaction, the transition state is a point on the minimum energy reaction pathway with maximum potential energy. Firstly, it is in the minimum energy pathway,so it is a minimum perpendicular to the reaction pathway. then, maximum potential energy appears at this point, means it is maximum alone the reaction pathway&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;. This sort of point are mathematically defined as a saddle point of a surface. &lt;br /&gt;
===Identification of transition state===&lt;br /&gt;
As the transition state can be represent by a saddle point, it is possible to apply mathematical methods&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt; of identifying stationary points to determine whether a stationary point represent the stationary point or not. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Mathematical method of identifying stationary points of a surface&lt;br /&gt;
! type of stationary points !! identification methond &lt;br /&gt;
|-&lt;br /&gt;
| local maximum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;lt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| local minimum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;gt; 0 &amp;lt;/math&amp;gt; &lt;br /&gt;
|-&lt;br /&gt;
| saddle point || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2}\frac {\partial^2 }{\partial y^2}-\frac {\partial^2 }{\partial xy}\frac {\partial^2 }{\partial yx} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
For a potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). In order to identify if a point with certain reaction coordinates represent the transition state or not, we can substitute the reaction coordinates into the function &amp;lt;math&amp;gt;\frac {\partial^2V }{\partial r_1^2}\frac {\partial^2V }{\partial r_2^2}-\frac {\partial^2V }{\partial r_1r_2y}\frac {\partial^2V }{\partial r_2r_1}&amp;lt;/math&amp;gt;. If the result is negative, it is the saddle point if the potential surface, and can represent the transition state. &lt;br /&gt;
==Question 2==&lt;br /&gt;
===Transition state position estimation===&lt;br /&gt;
For the reaction of a hydrogen atom collides with a hydrogen molecule at 180 degree to form a new hydrogen molecule and release an other hydrogen atom, consider there are only two degrees of freedom involved in the function of potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;), where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is the distance between the free atom and one end of the molecule, and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is the distance between the two H atoms originally in the hydrogen molecule. The system is symmetric, so r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are equal at the transition state. Secondly, for a stationary point, we have &amp;lt;math&amp;gt;\frac {\partial V }{\partial v_1}=\frac {\partial V}{\partial v_2}=0&amp;lt;/math&amp;gt;. The first derivative of potential is force. Therefore, in order to find the best estimation of the transition state. We need to run estimations with different r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, until we find the force alone the direction of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are both 0. The modelling starts from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=230pm(the initial distance between the free H atom and hydrogen molecule), and the best estimation is r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=90.775pm. &lt;br /&gt;
&lt;br /&gt;
==Question 3==&lt;br /&gt;
===Reaction trajectories calculation===&lt;br /&gt;
&lt;br /&gt;
==Question 4==&lt;br /&gt;
in this section A represent the original free H atom, B is the H atom in hydrogen molecule that collide with A, and C the H atom leaving the molecule after collision. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;/kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280|| Yes||The reactants successfully pass through the transition state and reaches the product. ||[[File:Animation1-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077|| No||The reactants cannot pass through the transition state, and bounce back to the reactants.  ||[[File:Animation2-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977|| Yes|| The reactants successfully pass through the transition state and reaches the product.||[[File:Animation3-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277|| No|| The reactants successfully pass through the transition state, however, they bounce back in to the reactants with a higher level of vibrational state.||[[File:Animation4-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477|| Yes||The reactants successfully pass through the transition state, then it bounce back once and enter the product side once again. The products formed are in a higher level vibrational state. ||[[File:Animation5-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;br /&gt;
1. Molecular Driving force&lt;br /&gt;
2. Chemistry math book&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811335</id>
		<title>MRD:cid-01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811335"/>
		<updated>2020-05-22T20:12:24Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Question 1 ==&lt;br /&gt;
===Mathematical definition of transition state===&lt;br /&gt;
When modelling a potential energy surface of a chemical reaction, the transition state is a point on the minimum energy reaction pathway with maximum potential energy. Firstly, it is in the minimum energy pathway,so it is a minimum perpendicular to the reaction pathway. then, maximum potential energy appears at this point, means it is maximum alone the reaction pathway&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;. This sort of point are mathematically defined as a saddle point of a surface. &lt;br /&gt;
===Identification of transition state===&lt;br /&gt;
As the transition state can be represent by a saddle point, it is possible to apply mathematical methods&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt; of identifying stationary points to determine whether a stationary point represent the stationary point or not. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Mathematical method of identifying stationary points of a surface&lt;br /&gt;
! type of stationary points !! identification methond &lt;br /&gt;
|-&lt;br /&gt;
| local maximum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;lt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| local minimum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;gt; 0 &amp;lt;/math&amp;gt; &lt;br /&gt;
|-&lt;br /&gt;
| saddle point || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2}\frac {\partial^2 }{\partial y^2}-\frac {\partial^2 }{\partial xy}\frac {\partial^2 }{\partial yx} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
For a potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). In order to identify if a point with certain reaction coordinates represent the transition state or not, we can substitute the reaction coordinates into the function &amp;lt;math&amp;gt;\frac {\partial^2V }{\partial r_1^2}\frac {\partial^2V }{\partial r_2^2}-\frac {\partial^2V }{\partial r_1r_2y}\frac {\partial^2V }{\partial r_2r_1}&amp;lt;/math&amp;gt;. If the result is negative, it is the saddle point if the potential surface, and can represent the transition state. &lt;br /&gt;
==Question 2==&lt;br /&gt;
===Transition state position estimation===&lt;br /&gt;
For the reaction of a hydrogen atom collides with a hydrogen molecule at 180 degree to form a new hydrogen molecule and release an other hydrogen atom, consider there are only two degrees of freedom involved in the function of potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;), where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is the distance between the free atom and one end of the molecule, and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is the distance between the two H atoms originally in the hydrogen molecule. The system is symmetric, so r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are equal at the transition state. Secondly, for a stationary point, we have &amp;lt;math&amp;gt;\frac {\partial V }{\partial v_1}=\frac {\partial V}{\partial v_2}=0&amp;lt;/math&amp;gt;. The first derivative of potential is force. Therefore, in order to find the best estimation of the transition state. We need to run estimations with different r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, until we find the force alone the direction of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are both 0. The modelling starts from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=230pm(the initial distance between the free H atom and hydrogen molecule), and the best estimation is r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=90.775pm. &lt;br /&gt;
&lt;br /&gt;
==Question 3==&lt;br /&gt;
===Reaction trajectories calculation===&lt;br /&gt;
&lt;br /&gt;
==Question 4==&lt;br /&gt;
in this section A represent the original free H atom, B is the H atom in hydrogen molecule that collide with A, and C the H atom leaving the molecule after collision. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt;kjmol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280|| Yes||The reactants successfully pass through the transition state and reaches the product. ||[[File:Animation1-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077|| No||The reactants cannot pass through the transition state, and bounce back to the reactants.  ||[[File:Animation2-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977|| Yes|| The reactants successfully pass through the transition state and reaches the product.||[[File:Animation3-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277|| No|| The reactants successfully pass through the transition state, however, they bounce back in to the reactants with a higher level of vibrational state.||[[File:Animation4-01554120.png|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477|| Yes||The reactants successfully pass through the transition state, then it bounce back once and enter the product side once again. The products formed are in a higher level vibrational state. ||[[File:Animation5-01554120.png|250px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;br /&gt;
1. Molecular Driving force&lt;br /&gt;
2. Chemistry math book&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Animation5-01554120.png&amp;diff=811309</id>
		<title>File:Animation5-01554120.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Animation5-01554120.png&amp;diff=811309"/>
		<updated>2020-05-22T20:05:19Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Animation4-01554120.png&amp;diff=811307</id>
		<title>File:Animation4-01554120.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Animation4-01554120.png&amp;diff=811307"/>
		<updated>2020-05-22T20:04:49Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Animation3-01554120.png&amp;diff=811305</id>
		<title>File:Animation3-01554120.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Animation3-01554120.png&amp;diff=811305"/>
		<updated>2020-05-22T20:04:23Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Animation2-01554120.png&amp;diff=811298</id>
		<title>File:Animation2-01554120.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Animation2-01554120.png&amp;diff=811298"/>
		<updated>2020-05-22T20:03:09Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: The second set of initial condition tested.&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The second set of initial condition tested.&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Animation1-01554120.png&amp;diff=811288</id>
		<title>File:Animation1-01554120.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Animation1-01554120.png&amp;diff=811288"/>
		<updated>2020-05-22T20:00:45Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: Jz13018 uploaded a new version of File:Animation1-01554120.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811285</id>
		<title>MRD:cid-01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811285"/>
		<updated>2020-05-22T20:00:21Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Question 1 ==&lt;br /&gt;
===Mathematical definition of transition state===&lt;br /&gt;
When modelling a potential energy surface of a chemical reaction, the transition state is a point on the minimum energy reaction pathway with maximum potential energy. Firstly, it is in the minimum energy pathway,so it is a minimum perpendicular to the reaction pathway. then, maximum potential energy appears at this point, means it is maximum alone the reaction pathway&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;. This sort of point are mathematically defined as a saddle point of a surface. &lt;br /&gt;
===Identification of transition state===&lt;br /&gt;
As the transition state can be represent by a saddle point, it is possible to apply mathematical methods&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt; of identifying stationary points to determine whether a stationary point represent the stationary point or not. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Mathematical method of identifying stationary points of a surface&lt;br /&gt;
! type of stationary points !! identification methond &lt;br /&gt;
|-&lt;br /&gt;
| local maximum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;lt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| local minimum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;gt; 0 &amp;lt;/math&amp;gt; &lt;br /&gt;
|-&lt;br /&gt;
| saddle point || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2}\frac {\partial^2 }{\partial y^2}-\frac {\partial^2 }{\partial xy}\frac {\partial^2 }{\partial yx} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
For a potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). In order to identify if a point with certain reaction coordinates represent the transition state or not, we can substitute the reaction coordinates into the function &amp;lt;math&amp;gt;\frac {\partial^2V }{\partial r_1^2}\frac {\partial^2V }{\partial r_2^2}-\frac {\partial^2V }{\partial r_1r_2y}\frac {\partial^2V }{\partial r_2r_1}&amp;lt;/math&amp;gt;. If the result is negative, it is the saddle point if the potential surface, and can represent the transition state. &lt;br /&gt;
==Question 2==&lt;br /&gt;
===Transition state position estimation===&lt;br /&gt;
For the reaction of a hydrogen atom collides with a hydrogen molecule at 180 degree to form a new hydrogen molecule and release an other hydrogen atom, consider there are only two degrees of freedom involved in the function of potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;), where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is the distance between the free atom and one end of the molecule, and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is the distance between the two H atoms originally in the hydrogen molecule. The system is symmetric, so r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are equal at the transition state. Secondly, for a stationary point, we have &amp;lt;math&amp;gt;\frac {\partial V }{\partial v_1}=\frac {\partial V}{\partial v_2}=0&amp;lt;/math&amp;gt;. The first derivative of potential is force. Therefore, in order to find the best estimation of the transition state. We need to run estimations with different r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, until we find the force alone the direction of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are both 0. The modelling starts from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=230pm(the initial distance between the free H atom and hydrogen molecule), and the best estimation is r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=90.775pm. &lt;br /&gt;
&lt;br /&gt;
==Question 3==&lt;br /&gt;
===Reaction trajectories calculation===&lt;br /&gt;
&lt;br /&gt;
==Question 4==&lt;br /&gt;
in this section A represent the original free H atom, B is the H atom in hydrogen molecule that collide with A, and C the H atom leaving the molecule after collision. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280|| Yes|| [[File:Animation-01554120.png]]||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077|| No|| ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977|| Yes|| ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277|| No|| ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477|| Yes|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;br /&gt;
1. Molecular Driving force&lt;br /&gt;
2. Chemistry math book&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Animation1-01554120.png&amp;diff=811277</id>
		<title>File:Animation1-01554120.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Animation1-01554120.png&amp;diff=811277"/>
		<updated>2020-05-22T19:58:41Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811275</id>
		<title>MRD:cid-01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811275"/>
		<updated>2020-05-22T19:58:20Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Question 1 ==&lt;br /&gt;
===Mathematical definition of transition state===&lt;br /&gt;
When modelling a potential energy surface of a chemical reaction, the transition state is a point on the minimum energy reaction pathway with maximum potential energy. Firstly, it is in the minimum energy pathway,so it is a minimum perpendicular to the reaction pathway. then, maximum potential energy appears at this point, means it is maximum alone the reaction pathway&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;. This sort of point are mathematically defined as a saddle point of a surface. &lt;br /&gt;
===Identification of transition state===&lt;br /&gt;
As the transition state can be represent by a saddle point, it is possible to apply mathematical methods&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt; of identifying stationary points to determine whether a stationary point represent the stationary point or not. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Mathematical method of identifying stationary points of a surface&lt;br /&gt;
! type of stationary points !! identification methond &lt;br /&gt;
|-&lt;br /&gt;
| local maximum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;lt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| local minimum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;gt; 0 &amp;lt;/math&amp;gt; &lt;br /&gt;
|-&lt;br /&gt;
| saddle point || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2}\frac {\partial^2 }{\partial y^2}-\frac {\partial^2 }{\partial xy}\frac {\partial^2 }{\partial yx} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
For a potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). In order to identify if a point with certain reaction coordinates represent the transition state or not, we can substitute the reaction coordinates into the function &amp;lt;math&amp;gt;\frac {\partial^2V }{\partial r_1^2}\frac {\partial^2V }{\partial r_2^2}-\frac {\partial^2V }{\partial r_1r_2y}\frac {\partial^2V }{\partial r_2r_1}&amp;lt;/math&amp;gt;. If the result is negative, it is the saddle point if the potential surface, and can represent the transition state. &lt;br /&gt;
==Question 2==&lt;br /&gt;
===Transition state position estimation===&lt;br /&gt;
For the reaction of a hydrogen atom collides with a hydrogen molecule at 180 degree to form a new hydrogen molecule and release an other hydrogen atom, consider there are only two degrees of freedom involved in the function of potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;), where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is the distance between the free atom and one end of the molecule, and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is the distance between the two H atoms originally in the hydrogen molecule. The system is symmetric, so r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are equal at the transition state. Secondly, for a stationary point, we have &amp;lt;math&amp;gt;\frac {\partial V }{\partial v_1}=\frac {\partial V}{\partial v_2}=0&amp;lt;/math&amp;gt;. The first derivative of potential is force. Therefore, in order to find the best estimation of the transition state. We need to run estimations with different r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, until we find the force alone the direction of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are both 0. The modelling starts from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=230pm(the initial distance between the free H atom and hydrogen molecule), and the best estimation is r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=90.775pm. &lt;br /&gt;
&lt;br /&gt;
==Question 3==&lt;br /&gt;
===Reaction trajectories calculation===&lt;br /&gt;
&lt;br /&gt;
==Question 4==&lt;br /&gt;
in this section A represent the original free H atom, B is the H atom in hydrogen molecule that collide with A, and C the H atom leaving the molecule after collision. &lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=1&lt;br /&gt;
! p&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! p&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/&amp;amp;nbsp;g.mol&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;.pm.fs&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; !! E&amp;lt;sub&amp;gt;tot&amp;lt;/sub&amp;gt; !! Reactive? !! Description of the dynamics !! Illustration of the trajectory&lt;br /&gt;
|-&lt;br /&gt;
| -2.56 || -5.1  || -414.280|| Yes|| ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -4.1  || -420.077|| No|| ||&lt;br /&gt;
|-&lt;br /&gt;
| -3.1  || -5.1  || -413.977|| Yes|| ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.1 || -357.277|| No|| ||&lt;br /&gt;
|-&lt;br /&gt;
| -5.1  || -10.6 || -349.477|| Yes|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;br /&gt;
1. Molecular Driving force&lt;br /&gt;
2. Chemistry math book&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811174</id>
		<title>MRD:cid-01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=811174"/>
		<updated>2020-05-22T19:32:03Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Question 1 ==&lt;br /&gt;
===Mathematical definition of transition state===&lt;br /&gt;
When modelling a potential energy surface of a chemical reaction, the transition state is a point on the minimum energy reaction pathway with maximum potential energy. Firstly, it is in the minimum energy pathway,so it is a minimum perpendicular to the reaction pathway. then, maximum potential energy appears at this point, means it is maximum alone the reaction pathway&amp;lt;sup&amp;gt;[1]&amp;lt;/sup&amp;gt;. This sort of point are mathematically defined as a saddle point of a surface. &lt;br /&gt;
===Identification of transition state===&lt;br /&gt;
As the transition state can be represent by a saddle point, it is possible to apply mathematical methods&amp;lt;sup&amp;gt;[2]&amp;lt;/sup&amp;gt; of identifying stationary points to determine whether a stationary point represent the stationary point or not. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Mathematical method of identifying stationary points of a surface&lt;br /&gt;
! type of stationary points !! identification methond &lt;br /&gt;
|-&lt;br /&gt;
| local maximum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;lt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| local minimum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;gt; 0 &amp;lt;/math&amp;gt; &lt;br /&gt;
|-&lt;br /&gt;
| saddle point || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2}\frac {\partial^2 }{\partial y^2}-\frac {\partial^2 }{\partial xy}\frac {\partial^2 }{\partial yx} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
For a potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;). In order to identify if a point with certain reaction coordinates represent the transition state or not, we can substitute the reaction coordinates into the function &amp;lt;math&amp;gt;\frac {\partial^2V }{\partial r_1^2}\frac {\partial^2V }{\partial r_2^2}-\frac {\partial^2V }{\partial r_1r_2y}\frac {\partial^2V }{\partial r_2r_1}&amp;lt;/math&amp;gt;. If the result is negative, it is the saddle point if the potential surface, and can represent the transition state. &lt;br /&gt;
==Question 2==&lt;br /&gt;
===Transition state position estimation===&lt;br /&gt;
For the reaction of a hydrogen atom collides with a hydrogen molecule at 180 degree to form a new hydrogen molecule and release an other hydrogen atom, consider there are only two degrees of freedom involved in the function of potential surface V(r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;), where r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; is the distance between the free atom and one end of the molecule, and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; is the distance between the two H atoms originally in the hydrogen molecule. The system is symmetric, so r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are equal at the transition state. Secondly, for a stationary point, we have &amp;lt;math&amp;gt;\frac {\partial V }{\partial v_1}=\frac {\partial V}{\partial v_2}=0&amp;lt;/math&amp;gt;. The first derivative of potential is force. Therefore, in order to find the best estimation of the transition state. We need to run estimations with different r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, until we find the force alone the direction of r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; and r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; are both 0. The modelling starts from r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=230pm(the initial distance between the free H atom and hydrogen molecule), and the best estimation is r&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=r&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=90.775pm. &lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;br /&gt;
1. Molecular Driving force&lt;br /&gt;
2. Chemistry math book&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=810943</id>
		<title>MRD:cid-01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=810943"/>
		<updated>2020-05-22T18:24:37Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Question 1 ==&lt;br /&gt;
===Mathematical definition of transition state===&lt;br /&gt;
When modelling a potential energy surface of a chemical reaction, the transition state is a point on the minimum energy reaction pathway with maximum potential energy. Firstly, it is in the minimum energy pathway,so it is a minimum perpendicular to the reaction pathway. then, maximum potential energy appears at this point, means it is maximum alone the reaction pathway. REFERENCE1. This sort of point are mathematically defined as a saddle point of a surface. &lt;br /&gt;
===Identification of transition state===&lt;br /&gt;
As the transition state can be represent by a saddle point, it is possible to apply mathematical methods of identifying stationary points to determine whether a stationary point represent the stationary point or not. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Mathematical method of identifying stationary points of a surface&lt;br /&gt;
! type of stationary points !! identification methond &lt;br /&gt;
|-&lt;br /&gt;
| local maximum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;lt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| local minimum || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2} &amp;gt; 0 &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial y^2} &amp;gt; 0 &amp;lt;/math&amp;gt; &lt;br /&gt;
|-&lt;br /&gt;
| saddle point || &amp;lt;math&amp;gt;\frac {\partial^2 }{\partial x^2}\frac {\partial^2 }{\partial y^2}-\frac {\partial^2 }{\partial xy}\frac {\partial^2 }{\partial yx} &amp;lt; 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
For a potential surface V(r_1, r_2). In order to identify if a point with certain reaction coordinates represent the transition state or not, we can substitute the reaction coordinates into the function &amp;lt;math&amp;gt;\frac {\partial^2V }{\partial r_1^2}\frac {\partial^2V }{\partial r_2^2}-\frac {\partial^2V }{\partial r_1r_2y}\frac {\partial^2V }{\partial r_2r_1}&amp;lt;/math&amp;gt;. If the result is negative, it is the saddle point if the potential surface, and can represent the transition state. &lt;br /&gt;
==Question 2==&lt;br /&gt;
===Estimation of transition state position===&lt;br /&gt;
===Explanation===&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=810853</id>
		<title>MRD:cid-01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MRD:cid-01554120&amp;diff=810853"/>
		<updated>2020-05-22T18:01:57Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: Created page with &amp;quot;==Question 1 == ===Mathematical definition of transition state=== When modelling a potential energy surface of a chemical reaction, the transition state is a point on the mini...&amp;quot;&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Question 1 ==&lt;br /&gt;
===Mathematical definition of transition state===&lt;br /&gt;
When modelling a potential energy surface of a chemical reaction, the transition state is a point on the minimum energy reaction pathway with maximum potential energy. Firstly, it is in the minimum energy pathway,so it is a minimum perpendicular to the reaction pathway. then, maximum potential energy appears at this point, means it is maximum alone the reaction pathway. REFERENCE1. This sort of point are mathematically defined as a saddle point of a surface. &lt;br /&gt;
===Identification of transition state===&lt;br /&gt;
As the transition state can be represent by a saddle point, it is possible to apply mathematical methods of identifying stationary points to determine whether a stationary point represent the stationary point or not. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|+ Mathematical method of identifying stationary points of a surface&lt;br /&gt;
! type of stationary points !! identification methond &lt;br /&gt;
|-&lt;br /&gt;
| local maximum || fxx&amp;lt;0, fyy&amp;lt;0 &lt;br /&gt;
|-&lt;br /&gt;
| local minimum || fxx&amp;gt;0, fyy&amp;gt;0 &lt;br /&gt;
|-&lt;br /&gt;
| saddle point || fxxfyy-f2xy&amp;lt;0&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
For a potential surface V(r1, r2). &lt;br /&gt;
==Question 2==&lt;br /&gt;
===Estimation of transition state position===&lt;br /&gt;
===Explanation===&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=754667</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=754667"/>
		<updated>2019-03-14T17:18:36Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: /* Transition metal complex */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&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; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.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;
The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
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&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
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=Hydrogen molecule analysis=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -1.15928020 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 0.60±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&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 &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; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.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;
The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
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| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
There will be only one absorption according to the 3N-5 rule for linear molecule. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
The two nitrogen atoms have same electronegativity, so the charge are evenly separated and both are 0 on each atom.&lt;br /&gt;
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=Transition metal complex=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
|-&lt;br /&gt;
| N-N bond length || 1.112Å&lt;br /&gt;
|-&lt;br /&gt;
| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
&lt;br /&gt;
Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy.&lt;br /&gt;
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=reaction energy of Haber-Bosch Process=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
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The reaction energy has a negative value, which suggests the product (ammonia) is more stable compare with the reactant (hydrogen and nitrogen).&lt;br /&gt;
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=Analysis of ammonium ion=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
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| point group|| C1&lt;br /&gt;
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| bond length|| 1.03±0.01Å&lt;br /&gt;
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| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
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| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
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| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibration modes according to the 3N-6 rule for non-linear molecules. Therer will be four distinguishable peaks on the spectrum as some of those modes are degenerated. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
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Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-NH4-orb1.png|left|thumb|Picture1. The lowest orbital of ammonium ion ]]&lt;br /&gt;
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Picture1: This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. This orbital doesn&#039;t contribute to the bonding. &lt;br /&gt;
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[[File:01554120-NH4-orb2.png|left|thumb|Picture2. The 2nd orbital of ammonium ion ]]&lt;br /&gt;
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Picture2: This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. This orbital contributes to the bonding. &lt;br /&gt;
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[[File:01554120-NH4-orb3.png|left|thumb|Picture3. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This one of the bonding orbitals of ammonium ion, it is form by a nitrogen 2p orbital over with a hydrogen AO. This orbital contributes to the bonding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb5.png|left|thumb|Picture4. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the HOMO of the ammonium ion, it is the anti-bonding orbital of the overlap between 2s orbital of nitrogen and one of the four hydrogen atomic orbitals. Due to stablisation, the HOMO is quite close in energy (-0.82457 a.u.) with the previous 2 orbitals, not like the HOMO of ammonium molecule. This orbital contributes to the bonding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb6.png|left|thumb|Picture5. The 6th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is the LUMO of the ammonium ion, its energy (-0.20998 a.u.)is higher than the previous three molecular orbitals (approx-0.825 a.u.). and it is made from a p orbital of nitrogen and one of the four 4H atomic orbitals. This orbital doesn&#039;t contribute to the bonding.&lt;br /&gt;
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=Analysis of CO molecule=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
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| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
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| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&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; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Spectroscopy analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-CO-vib.png|thumb|left|spectroscopic data of carbon monoxide molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2209 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 67 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[01554120-CO-VM.png|150px]] &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-CO-charge.png|200px|left|thumb|Atomic charge data of carbon monoxide molecule.]]&lt;br /&gt;
&lt;br /&gt;
As carbon and oxygen atoms have different electronegativity, charge will distributed unevenly on two atoms, and as oxygen is more electronegative, it will carry the negative charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;molecular orbital of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-COMO1.png|left|thumb|Picture1. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture1: This is the bonding orbital (3σ) formed by the overlap of two 2s orbital of carbon and oxygen atom, its energy is -1.15791 a.u. This orbital contributes to the bonding. &lt;br /&gt;
[[File:01554120-COMO2.png|left|thumb|Picture1. The 4th orbital of ammonium ion ]]&lt;br /&gt;
Picture2: This is the 4σ orbital of the molecule, it is made by two head to head 2p orbitals overlap in phase. Its energy is -0.57004a.u. This orbital contributes to the bonding. &lt;br /&gt;
[[File:01554120-COMO3.png|left|thumb|Picture1. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This is one of the degenerated 1π orbitals of the molecule, it is formed by two 2p orbital of each atom in phase parallel overlap and its energy is -0.46743 a.u. This orbital contributes to the bonding. &lt;br /&gt;
[[File:01554120-COMO4.png|left|thumb|Picture1. The 7th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the 5σ orbital of the molecule, it is also the HOMO (energy=-0.37145). it is made by two out of phase 2s orbital from each atom overlap. This orbital doesn&#039;t contribute to the bonding. &lt;br /&gt;
[[File:01554120-COMO5.png|left|thumb|Picture1. The 8th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is one of the degenerated 2π orbital of the molecule, it is also the LUMO (energy=-0.2177 a.u.). it is made by two out of phase 2p from each atom orbital parallel overlap. This orbital doesn&#039;t contribute to the bonding, as no electrons in it.&lt;br /&gt;
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=Marking=&lt;br /&gt;
 &lt;br /&gt;
Note: All grades and comments are provisional and subjecct to change until your grades are officially returned via blackboard. Please do not contact anyone about anything to do with the marking of this lab until you have recieved your grade from blackboard.&lt;br /&gt;
 &lt;br /&gt;
==Wiki structure and presentation 1/1 ==&lt;br /&gt;
 &lt;br /&gt;
Is your wiki page clear and easy to follow, with consistent formatting?&lt;br /&gt;
 &lt;br /&gt;
YES -however, you could have used subsections more efficiently&lt;br /&gt;
 &lt;br /&gt;
Do you effectively use tables, figures and subheadings to communicate your work?&lt;br /&gt;
 &lt;br /&gt;
YES&lt;br /&gt;
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==NH3 0.5/1 ==&lt;br /&gt;
 &lt;br /&gt;
Have you completed the calculation and given a link to the file?&lt;br /&gt;
 &lt;br /&gt;
YES&lt;br /&gt;
 &lt;br /&gt;
Have you included summary and item tables in your wiki?&lt;br /&gt;
 &lt;br /&gt;
YES&lt;br /&gt;
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Have you included a 3d jmol file or an image of the finished structure?&lt;br /&gt;
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YES&lt;br /&gt;
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Have you included the bond lengths and angles asked for?&lt;br /&gt;
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YES&lt;br /&gt;
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Have you included the “display vibrations” table?&lt;br /&gt;
 &lt;br /&gt;
YES&lt;br /&gt;
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Have you added a table to your wiki listing the wavenumber and intensity of each vibration?&lt;br /&gt;
 &lt;br /&gt;
YES&lt;br /&gt;
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Did you do the optional extra of adding images of the vibrations?&lt;br /&gt;
 &lt;br /&gt;
YES&lt;br /&gt;
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Have you included answers to the questions about vibrations and charges in the lab script?&lt;br /&gt;
 &lt;br /&gt;
YES - You identified the requirement for degenerate vibrations correctly. However, you made a mistake regarding the degenerate modes. Modes 2 and 3 are degenerate, not 3 and 4. You stated mode 4 to be the umbrella mode but from optical inspection of this mode t is obvious this is a symmetric stretch of all three NH bonds. Mode 1 is the umbrella mode as it resembles the motion when opening an umbrella. You correctly stated that there are two sets of degenerate modes - this explains a spectrum with 4 peaks. However there are only 2 peaks visible as peaks 4, 5 and 6 are of too low an intensity to be visible.&lt;br /&gt;
 &lt;br /&gt;
== N2 and H2 0.5/0.5 ==&lt;br /&gt;
 &lt;br /&gt;
Have you completed the calculations and included all relevant information? (summary, item table, structural information, jmol image, vibrations and charges)&lt;br /&gt;
 &lt;br /&gt;
YES - however you stated H2 to be a uniatomic molecule, this would be one atom! H2 is a diatomic with both atoms being the same.&lt;br /&gt;
 &lt;br /&gt;
==Crystal structure comparison 0.5/0.5 ==&lt;br /&gt;
 &lt;br /&gt;
Have you included a link to a structure from the CCDC that includes a coordinated N2 or H2 molecule?  &lt;br /&gt;
 &lt;br /&gt;
YES&lt;br /&gt;
 &lt;br /&gt;
Have you compared your optimised bond distance to the crystal structure bond distance?&lt;br /&gt;
 &lt;br /&gt;
YES&lt;br /&gt;
 &lt;br /&gt;
==Haber-Bosch reaction energy calculation 0.5/1==&lt;br /&gt;
 &lt;br /&gt;
Have you correctly calculated the energies asked for? ΔE=2*E(NH3)-[E(N2)+3*E(H2)]&lt;br /&gt;
 &lt;br /&gt;
NO - The reported number of H2 is incorrect by 0.2 a.u., although the linked .log file contains the right energy for optimised H2. This results in a wrong overall reaction energy.&lt;br /&gt;
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Have you reported your answers to the correct number of decimal places?&lt;br /&gt;
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YES&lt;br /&gt;
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Do your energies have the correct +/- sign?&lt;br /&gt;
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YES&lt;br /&gt;
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Have you answered the question, Identify which is more stable the gaseous reactants or the ammonia product?&lt;br /&gt;
 &lt;br /&gt;
YES&lt;br /&gt;
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== Your choice of small molecule 2.5/5 ==&lt;br /&gt;
 &lt;br /&gt;
Have you completed the calculation and included all relevant information?&lt;br /&gt;
 &lt;br /&gt;
YES - however the point group of NH4+ is expected to be Td rather than C1.&lt;br /&gt;
&lt;br /&gt;
You tried to comment on the vibrations. You missed to state how many sets of degenerate modes were calculated and which modes are included to these sets. The modes 1-3, 4 &amp;amp;5 and 7-9 are degenerate . This would explain a spectrum with 4 peaks. However the intensities of the modes 4, 5 and 6 are too low in intensity to be observed experimentally. Therefore only two peaks will be seen in an experimental spectrum. &lt;br /&gt;
 &lt;br /&gt;
Have you added information about MOs and charges on atoms?&lt;br /&gt;
 &lt;br /&gt;
You have done a good job of presenting this information, well done!&lt;br /&gt;
&lt;br /&gt;
In most cases you stated the contributing AOs correctly and only missed to mention them explicitly once.&lt;br /&gt;
You missed to state which orbital is occupied/non-occupied.&lt;br /&gt;
The MOs 3-5 should all be degenerate and all bonding MOs. This discrepancy probably derives from the C1 point group of your ammonium ion. &lt;br /&gt;
The LUMO has no contribution from a p orbital. It is an ou-of-phase combination of the 2s on N and the 1s on the Hs and resembles a non-bonding MO with an internal node.&lt;br /&gt;
 &lt;br /&gt;
== Independence 1/1 ==&lt;br /&gt;
 &lt;br /&gt;
If you have finished everything else and have spare time in the lab you could:&lt;br /&gt;
Check one of your results against the literature, or&lt;br /&gt;
Do an extra calculation on another small molecule, or&lt;br /&gt;
 &lt;br /&gt;
YES - well done!&lt;br /&gt;
 &lt;br /&gt;
Do some deeper analysis on your results so far&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752277</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752277"/>
		<updated>2019-03-08T16:39:03Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
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| calculation method || RB3LYP &lt;br /&gt;
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| basis set|| 6-31G(d,p)&lt;br /&gt;
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| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
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| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
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 &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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
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| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
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| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
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| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
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There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
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&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
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=Hydrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
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| calculation method || RB3LYP &lt;br /&gt;
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| basis set|| 6-31G(d,p)&lt;br /&gt;
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| final energy|| -1.15928020 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
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| bond length|| 0.60±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&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 &amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
There will be only one absorption according to the 3N-5 rule for linear molecule. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
The two nitrogen atoms have same electronegativity, so the charge are evenly separated and both are 0 on each atom.&lt;br /&gt;
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=Transition metal complex=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
|-&lt;br /&gt;
| N-N bond length || 1.112Å&lt;br /&gt;
|-&lt;br /&gt;
| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
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Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
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=reaction energy of Haber-Bosch Process=&lt;br /&gt;
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&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
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The reaction energy has a negative value, which suggests the product (ammonia) is more stable compare with the reactant (hydrogen and nitrogen).&lt;br /&gt;
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=Analysis of ammonium ion=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C1&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.03±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.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;
The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibration modes according to the 3N-6 rule for non-linear molecules. Therer will be four distinguishable peaks on the spectrum as some of those modes are degenerated. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
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Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-NH4-orb1.png|left|thumb|Picture1. The lowest orbital of ammonium ion ]]&lt;br /&gt;
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Picture1: This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. This orbital doesn&#039;t contribute to the bonding. &lt;br /&gt;
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[[File:01554120-NH4-orb2.png|left|thumb|Picture2. The 2nd orbital of ammonium ion ]]&lt;br /&gt;
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Picture2: This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. This orbital contributes to the bonding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb3.png|left|thumb|Picture3. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This one of the bonding orbitals of ammonium ion, it is form by a nitrogen 2p orbital over with a hydrogen AO. This orbital contributes to the bonding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb5.png|left|thumb|Picture4. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the HOMO of the ammonium ion, it is the anti-bonding orbital of the overlap between 2s orbital of nitrogen and one of the four hydrogen atomic orbitals. Due to stablisation, the HOMO is quite close in energy (-0.82457 a.u.) with the previous 2 orbitals, not like the HOMO of ammonium molecule. This orbital contributes to the bonding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb6.png|left|thumb|Picture5. The 6th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is the LUMO of the ammonium ion, its energy (-0.20998 a.u.)is higher than the previous three molecular orbitals (approx-0.825 a.u.). and it is made from a p orbital of nitrogen and one of the four 4H atomic orbitals. This orbital doesn&#039;t contribute to the bonding.&lt;br /&gt;
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=Analysis of CO molecule=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.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;
The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Spectroscopy analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-CO-vib.png|thumb|left|spectroscopic data of carbon monoxide molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2209 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 67 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[01554120-CO-VM.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-CO-charge.png|200px|left|thumb|Atomic charge data of carbon monoxide molecule.]]&lt;br /&gt;
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As carbon and oxygen atoms have different electronegativity, charge will distributed unevenly on two atoms, and as oxygen is more electronegative, it will carry the negative charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;molecular orbital of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-COMO1.png|left|thumb|Picture1. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture1: This is the bonding orbital (3σ) formed by the overlap of two 2s orbital of carbon and oxygen atom, its energy is -1.15791 a.u. This orbital contributes to the bonding. &lt;br /&gt;
[[File:01554120-COMO2.png|left|thumb|Picture1. The 4th orbital of ammonium ion ]]&lt;br /&gt;
Picture2: This is the 4σ orbital of the molecule, it is made by two head to head 2p orbitals overlap in phase. Its energy is -0.57004a.u. This orbital contributes to the bonding. &lt;br /&gt;
[[File:01554120-COMO3.png|left|thumb|Picture1. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This is one of the degenerated 1π orbitals of the molecule, it is formed by two 2p orbital of each atom in phase parallel overlap and its energy is -0.46743 a.u. This orbital contributes to the bonding. &lt;br /&gt;
[[File:01554120-COMO4.png|left|thumb|Picture1. The 7th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the 5σ orbital of the molecule, it is also the HOMO (energy=-0.37145). it is made by two out of phase 2s orbital from each atom overlap. This orbital doesn&#039;t contribute to the bonding. &lt;br /&gt;
[[File:01554120-COMO5.png|left|thumb|Picture1. The 8th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is one of the degenerated 2π orbital of the molecule, it is also the LUMO (energy=-0.2177 a.u.). it is made by two out of phase 2p from each atom orbital parallel overlap. This orbital doesn&#039;t contribute to the bonding, as no electrons in it.&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752276</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752276"/>
		<updated>2019-03-08T16:34:10Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
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 &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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&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; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.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;
The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
&lt;br /&gt;
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=Hydrogen molecule analysis=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -1.15928020 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 0.60±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&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 &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; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.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;
The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
There will be only one absorption according to the 3N-5 rule for linear molecule. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
The two nitrogen atoms have same electronegativity, so the charge are evenly separated and both are 0 on each atom.&lt;br /&gt;
&lt;br /&gt;
=Transition metal complex=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
|-&lt;br /&gt;
| N-N bond length || 1.112Å&lt;br /&gt;
|-&lt;br /&gt;
| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
&lt;br /&gt;
Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
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=reaction energy of Haber-Bosch Process=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The reaction energy has a negative value, which suggests the product (ammonia) is more stable compare with the reactant (hydrogen and nitrogen).&lt;br /&gt;
&lt;br /&gt;
=Analysis of ammonium ion=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C1&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.03±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibration modes according to the 3N-6 rule for non-linear molecules. Therer will be four distinguishable peaks on the spectrum as some of those modes are degenerated. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
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Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-NH4-orb1.png|left|thumb|Picture1. The lowest orbital of ammonium ion ]]&lt;br /&gt;
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Picture1: This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. This orbital doesn&#039;t contribute to the bonding. &lt;br /&gt;
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[[File:01554120-NH4-orb2.png|left|thumb|Picture2. The 2nd orbital of ammonium ion ]]&lt;br /&gt;
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Picture2: This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. This orbital contributes to the bonding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb3.png|left|thumb|Picture3. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This one of the bonding orbitals of ammonium ion, it is form by a nitrogen 2p orbital over with a hydrogen AO. This orbital contributes to the bonding. &lt;br /&gt;
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[[File:01554120-NH4-orb5.png|left|thumb|Picture4. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the HOMO of the ammonium ion, it is the anti-bonding orbital of the overlap between 2s orbital of nitrogen and one of the four hydrogen atomic orbitals. Due to stablisation, the HOMO is quite close in energy (-0.82457 a.u.) with the previous 2 orbitals, not like the HOMO of ammonium molecule. This orbital contributes to the bonding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb6.png|left|thumb|Picture5. The 6th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is the LUMO of the ammonium ion, its energy (-0.20998 a.u.)is higher than the previous three molecular orbitals (approx-0.825 a.u.). and it is made from a p orbital of nitrogen and one of the four 4H atomic orbitals. This orbital doesn&#039;t contribute to the bonding.&lt;br /&gt;
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=Analysis of CO molecule=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.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;
The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Spectroscopy analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-CO-vib.png|thumb|left|spectroscopic data of carbon monoxide molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2209 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 67 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[01554120-CO-VM.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-CO-charge.png|200px|thumb|Atomic charge data of carbon monoxide molecule.]]&lt;br /&gt;
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&amp;lt;b&amp;gt;molecular orbital of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-COMO1.png|left|thumb|Picture1. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture1: This is the bonding orbital (3σ) formed by the overlap of two 2s orbital of carbon and oxygen atom, its energy is -1.15791 a.u. This orbital contributes to the bonding. &lt;br /&gt;
[[File:01554120-COMO2.png|left|thumb|Picture1. The 4th orbital of ammonium ion ]]&lt;br /&gt;
Picture2: This is the 4σ orbital of the molecule, it is made by two head to head 2p orbitals overlap in phase. Its energy is -0.57004a.u. This orbital contributes to the bonding. &lt;br /&gt;
[[File:01554120-COMO3.png|left|thumb|Picture1. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This is one of the degenerated 1π orbitals of the molecule, it is formed by two 2p orbital of each atom in phase parallel overlap and its energy is -0.46743 a.u. This orbital contributes to the bonding. &lt;br /&gt;
[[File:01554120-COMO4.png|left|thumb|Picture1. The 7th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the 5σ orbital of the molecule, it is also the HOMO (energy=-0.37145). it is made by two out of phase 2s orbital from each atom overlap. This orbital doesn&#039;t contribute to the bonding. &lt;br /&gt;
[[File:01554120-COMO5.png|left|thumb|Picture1. The 8th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is one of the degenerated 2π orbital of the molecule, it is also the LUMO (energy=-0.2177 a.u.). it is made by two out of phase 2p from each atom orbital parallel overlap. This orbital doesn&#039;t contribute to the bonding, as no electrons in it.&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752274</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752274"/>
		<updated>2019-03-08T16:32:02Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: /* Analysis of ammonium ion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
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| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
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| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
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 &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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.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;
The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
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| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
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| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
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&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
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=Hydrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
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| calculation method || RB3LYP &lt;br /&gt;
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| basis set|| 6-31G(d,p)&lt;br /&gt;
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| final energy|| -1.15928020 a.u.&lt;br /&gt;
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| point group|| D∞h&lt;br /&gt;
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| bond length|| 0.60±0.01Å&lt;br /&gt;
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&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 &amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
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| wavenumber/cm-1|| 4466 &lt;br /&gt;
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| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
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| calculation method || RB3LYP &lt;br /&gt;
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| basis set|| 6-31G(d,p)&lt;br /&gt;
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| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 &lt;br /&gt;
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| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
There will be only one absorption according to the 3N-5 rule for linear molecule. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
The two nitrogen atoms have same electronegativity, so the charge are evenly separated and both are 0 on each atom.&lt;br /&gt;
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=Transition metal complex=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
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| Code|| BARTOF&lt;br /&gt;
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| N-N bond length || 1.112Å&lt;br /&gt;
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| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
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Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
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=reaction energy of Haber-Bosch Process=&lt;br /&gt;
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&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
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The reaction energy has a negative value, which suggests the product (ammonia) is more stable compare with the reactant (hydrogen and nitrogen).&lt;br /&gt;
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=Analysis of ammonium ion=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C1&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.03±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.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;
The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibration modes according to the 3N-6 rule for non-linear molecules. Therer will be four distinguishable peaks on the spectrum as some of those modes are degenerated. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb1.png|left|thumb|Picture1. The lowest orbital of ammonium ion ]]&lt;br /&gt;
&lt;br /&gt;
Picture1: This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. This orbital doesn&#039;t contribute to the bonding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb2.png|left|thumb|Picture2. The 2nd orbital of ammonium ion ]]&lt;br /&gt;
&lt;br /&gt;
Picture2: This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. This orbital contributes to the bonding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb3.png|left|thumb|Picture3. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This one of the bonding orbitals of ammonium ion, it is form by a nitrogen 2p orbital over with a hydrogen AO. This orbital contributes to the bonding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb5.png|left|thumb|Picture4. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the HOMO of the ammonium ion, it is the anti-bonding orbital of the overlap between 2s orbital of nitrogen and one of the four hydrogen atomic orbitals. Due to stablisation, the HOMO is quite close in energy (-0.82457 a.u.) with the previous 2 orbitals, not like the HOMO of ammonium molecule. This orbital contributes to the bonding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb6.png|left|thumb|Picture5. The 6th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is the LUMO of the ammonium ion, its energy (-0.20998 a.u.)is higher than the previous three molecular orbitals (approx-0.825 a.u.). and it is made from a p orbital of nitrogen and one of the four 4H atomic orbitals. This orbital doesn&#039;t contribute to the bonding.&lt;br /&gt;
&lt;br /&gt;
=Analysis of CO molecule=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&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; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.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;
The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Spectroscopy analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-CO-vib.png|thumb|left|spectroscopic data of carbon monoxide molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2209 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 67 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[01554120-CO-VM.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-CO-charge.png|200px|thumb|Atomic charge data of carbon monoxide molecule.]]&lt;br /&gt;
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&amp;lt;b&amp;gt;molecular orbital of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-COMO1.png|left|thumb|Picture1. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture1: This is the bonding orbital (3σ) formed by the overlap of two 2s orbital of carbon and oxygen atom, its energy is -1.15791 a.u.&lt;br /&gt;
[[File:01554120-COMO2.png|left|thumb|Picture1. The 4th orbital of ammonium ion ]]&lt;br /&gt;
Picture2: This is the 4σ orbital of the molecule, it is made by two head to head 2p orbitals overlap in phase. Its energy is -0.57004a.u. &lt;br /&gt;
[[File:01554120-COMO3.png|left|thumb|Picture1. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This is one of the degenerated 1π orbitals of the molecule, it is formed by two 2p orbital of each atom in phase parallel overlap and its energy is -0.46743 a.u. &lt;br /&gt;
[[File:01554120-COMO4.png|left|thumb|Picture1. The 7th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the 5σ orbital of the molecule, it is also the HOMO (energy=-0.37145). it is made by two out of phase 2s orbital from each atom overlap. &lt;br /&gt;
[[File:01554120-COMO5.png|left|thumb|Picture1. The 8th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is one of the degenerated 2π orbital of the molecule, it is also the LUMO (energy=-0.2177 a.u.). it is made by two out of phase 2p from each atom orbital parallel overlap.&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752273</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752273"/>
		<updated>2019-03-08T16:25:11Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: /* reaction energy of Haber-Bosch Process */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
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 &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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.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;
The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
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&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
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=Hydrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -1.15928020 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 0.60±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&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 &amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
There will be only one absorption according to the 3N-5 rule for linear molecule. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
The two nitrogen atoms have same electronegativity, so the charge are evenly separated and both are 0 on each atom.&lt;br /&gt;
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=Transition metal complex=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
|-&lt;br /&gt;
| N-N bond length || 1.112Å&lt;br /&gt;
|-&lt;br /&gt;
| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
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Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
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=reaction energy of Haber-Bosch Process=&lt;br /&gt;
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&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
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The reaction energy has a negative value, which suggests the product (ammonia) is more stable compare with the reactant (hydrogen and nitrogen).&lt;br /&gt;
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=Analysis of ammonium ion=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C1&lt;br /&gt;
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| bond length|| 1.03±0.01Å&lt;br /&gt;
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| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibrational modes for ammonium ion. &lt;br /&gt;
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[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
There are 9 vibration modes according to the 3N-6 rule for non-linear molecules. Therer will be four distinguishable peaks on the spectrum as some of those modes are degenerated&lt;br /&gt;
&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
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Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-NH4-orb1.png|left|thumb|Picture1. The lowest orbital of ammonium ion ]]&lt;br /&gt;
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Picture1: This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. &lt;br /&gt;
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[[File:01554120-NH4-orb2.png|left|thumb|Picture2. The 2nd orbital of ammonium ion ]]&lt;br /&gt;
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Picture2: This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. &lt;br /&gt;
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[[File:01554120-NH4-orb3.png|left|thumb|Picture3. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This one of the bonding orbitals of ammonium ion, it is form by a nitrogen 2p orbital over with a hydrogen AO, &lt;br /&gt;
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[[File:01554120-NH4-orb5.png|left|thumb|Picture4. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the HOMO of the ammonium ion, it is the anti-bonding orbital of the overlap between 2s orbital of nitrogen and one of the four hydrogen atomic orbitals. Due to stablisation, the HOMO is quite close in energy (-0.82457 a.u.) with the previous 2 orbitals, not like the HOMO of ammonium molecule. &lt;br /&gt;
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[[File:01554120-NH4-orb6.png|left|thumb|Picture5. The 6th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is the LUMO of the ammonium ion, its energy (-0.20998 a.u.)is higher than the previous three molecular orbitals (approx-0.825 a.u.). and it is made from a p orbital of nitrogen and one of the four 4H atomic orbitals.&lt;br /&gt;
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=Analysis of CO molecule=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| CO&lt;br /&gt;
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| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
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| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
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| bond length|| 1.14±0.01Å&lt;br /&gt;
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&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Spectroscopy analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-CO-vib.png|thumb|left|spectroscopic data of carbon monoxide molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 &lt;br /&gt;
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| wavenumber/cm-1|| 2209 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 67 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[01554120-CO-VM.png|150px]] &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-CO-charge.png|200px|thumb|Atomic charge data of carbon monoxide molecule.]]&lt;br /&gt;
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&amp;lt;b&amp;gt;molecular orbital of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-COMO1.png|left|thumb|Picture1. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture1: This is the bonding orbital (3σ) formed by the overlap of two 2s orbital of carbon and oxygen atom, its energy is -1.15791 a.u.&lt;br /&gt;
[[File:01554120-COMO2.png|left|thumb|Picture1. The 4th orbital of ammonium ion ]]&lt;br /&gt;
Picture2: This is the 4σ orbital of the molecule, it is made by two head to head 2p orbitals overlap in phase. Its energy is -0.57004a.u. &lt;br /&gt;
[[File:01554120-COMO3.png|left|thumb|Picture1. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This is one of the degenerated 1π orbitals of the molecule, it is formed by two 2p orbital of each atom in phase parallel overlap and its energy is -0.46743 a.u. &lt;br /&gt;
[[File:01554120-COMO4.png|left|thumb|Picture1. The 7th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the 5σ orbital of the molecule, it is also the HOMO (energy=-0.37145). it is made by two out of phase 2s orbital from each atom overlap. &lt;br /&gt;
[[File:01554120-COMO5.png|left|thumb|Picture1. The 8th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is one of the degenerated 2π orbital of the molecule, it is also the LUMO (energy=-0.2177 a.u.). it is made by two out of phase 2p from each atom orbital parallel overlap.&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752271</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752271"/>
		<updated>2019-03-08T16:23:51Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: /* Nitrogen molecule analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
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 &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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.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;
The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
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| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
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&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
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=Hydrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -1.15928020 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 0.60±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&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 &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; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.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;
The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
There will be only one absorption according to the 3N-5 rule for linear molecule. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
The two nitrogen atoms have same electronegativity, so the charge are evenly separated and both are 0 on each atom.&lt;br /&gt;
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=Transition metal complex=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
|-&lt;br /&gt;
| N-N bond length || 1.112Å&lt;br /&gt;
|-&lt;br /&gt;
| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
&lt;br /&gt;
Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
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=reaction energy of Haber-Bosch Process=&lt;br /&gt;
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&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
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=Analysis of ammonium ion=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C1&lt;br /&gt;
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| bond length|| 1.03±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibrational modes for ammonium ion. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
There are 9 vibration modes according to the 3N-6 rule for non-linear molecules. Therer will be four distinguishable peaks on the spectrum as some of those modes are degenerated&lt;br /&gt;
&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
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Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-NH4-orb1.png|left|thumb|Picture1. The lowest orbital of ammonium ion ]]&lt;br /&gt;
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Picture1: This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. &lt;br /&gt;
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[[File:01554120-NH4-orb2.png|left|thumb|Picture2. The 2nd orbital of ammonium ion ]]&lt;br /&gt;
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Picture2: This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb3.png|left|thumb|Picture3. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This one of the bonding orbitals of ammonium ion, it is form by a nitrogen 2p orbital over with a hydrogen AO, &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb5.png|left|thumb|Picture4. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the HOMO of the ammonium ion, it is the anti-bonding orbital of the overlap between 2s orbital of nitrogen and one of the four hydrogen atomic orbitals. Due to stablisation, the HOMO is quite close in energy (-0.82457 a.u.) with the previous 2 orbitals, not like the HOMO of ammonium molecule. &lt;br /&gt;
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[[File:01554120-NH4-orb6.png|left|thumb|Picture5. The 6th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is the LUMO of the ammonium ion, its energy (-0.20998 a.u.)is higher than the previous three molecular orbitals (approx-0.825 a.u.). and it is made from a p orbital of nitrogen and one of the four 4H atomic orbitals.&lt;br /&gt;
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=Analysis of CO molecule=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Spectroscopy analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-CO-vib.png|thumb|left|spectroscopic data of carbon monoxide molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 &lt;br /&gt;
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| wavenumber/cm-1|| 2209 &lt;br /&gt;
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| Symmetry || SG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 67 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[01554120-CO-VM.png|150px]] &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-CO-charge.png|200px|thumb|Atomic charge data of carbon monoxide molecule.]]&lt;br /&gt;
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&amp;lt;b&amp;gt;molecular orbital of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-COMO1.png|left|thumb|Picture1. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture1: This is the bonding orbital (3σ) formed by the overlap of two 2s orbital of carbon and oxygen atom, its energy is -1.15791 a.u.&lt;br /&gt;
[[File:01554120-COMO2.png|left|thumb|Picture1. The 4th orbital of ammonium ion ]]&lt;br /&gt;
Picture2: This is the 4σ orbital of the molecule, it is made by two head to head 2p orbitals overlap in phase. Its energy is -0.57004a.u. &lt;br /&gt;
[[File:01554120-COMO3.png|left|thumb|Picture1. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This is one of the degenerated 1π orbitals of the molecule, it is formed by two 2p orbital of each atom in phase parallel overlap and its energy is -0.46743 a.u. &lt;br /&gt;
[[File:01554120-COMO4.png|left|thumb|Picture1. The 7th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the 5σ orbital of the molecule, it is also the HOMO (energy=-0.37145). it is made by two out of phase 2s orbital from each atom overlap. &lt;br /&gt;
[[File:01554120-COMO5.png|left|thumb|Picture1. The 8th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is one of the degenerated 2π orbital of the molecule, it is also the LUMO (energy=-0.2177 a.u.). it is made by two out of phase 2p from each atom orbital parallel overlap.&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752269</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752269"/>
		<updated>2019-03-08T16:21:39Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
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&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
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 &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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
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| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
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| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
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&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
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=Hydrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
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| calculation method || RB3LYP &lt;br /&gt;
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| basis set|| 6-31G(d,p)&lt;br /&gt;
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| final energy|| -1.15928020 a.u.&lt;br /&gt;
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| point group|| D∞h&lt;br /&gt;
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| bond length|| 0.60±0.01Å&lt;br /&gt;
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&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 &amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
There will be only one absorption according to the 3N-5 rule for linear molecule. &lt;br /&gt;
&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
The two nitrogen atoms have same electronegativity, so the charge are evenly separated and both are 0 on each atom. &lt;br /&gt;
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=Transition metal complex=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
|-&lt;br /&gt;
| N-N bond length || 1.112Å&lt;br /&gt;
|-&lt;br /&gt;
| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
&lt;br /&gt;
Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
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=reaction energy of Haber-Bosch Process=&lt;br /&gt;
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&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
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=Analysis of ammonium ion=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C1&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.03±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibrational modes for ammonium ion. &lt;br /&gt;
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[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
There are 9 vibration modes according to the 3N-6 rule for non-linear molecules. Therer will be four distinguishable peaks on the spectrum as some of those modes are degenerated&lt;br /&gt;
&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
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Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-NH4-orb1.png|left|thumb|Picture1. The lowest orbital of ammonium ion ]]&lt;br /&gt;
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Picture1: This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. &lt;br /&gt;
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[[File:01554120-NH4-orb2.png|left|thumb|Picture2. The 2nd orbital of ammonium ion ]]&lt;br /&gt;
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Picture2: This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. &lt;br /&gt;
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[[File:01554120-NH4-orb3.png|left|thumb|Picture3. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This one of the bonding orbitals of ammonium ion, it is form by a nitrogen 2p orbital over with a hydrogen AO, &lt;br /&gt;
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[[File:01554120-NH4-orb5.png|left|thumb|Picture4. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the HOMO of the ammonium ion, it is the anti-bonding orbital of the overlap between 2s orbital of nitrogen and one of the four hydrogen atomic orbitals. Due to stablisation, the HOMO is quite close in energy (-0.82457 a.u.) with the previous 2 orbitals, not like the HOMO of ammonium molecule. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb6.png|left|thumb|Picture5. The 6th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is the LUMO of the ammonium ion, its energy (-0.20998 a.u.)is higher than the previous three molecular orbitals (approx-0.825 a.u.). and it is made from a p orbital of nitrogen and one of the four 4H atomic orbitals.&lt;br /&gt;
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=Analysis of CO molecule=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.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;
The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Spectroscopy analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-CO-vib.png|thumb|left|spectroscopic data of carbon monoxide molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2209 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 67 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[01554120-CO-VM.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-CO-charge.png|200px|thumb|Atomic charge data of carbon monoxide molecule.]]&lt;br /&gt;
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&amp;lt;b&amp;gt;molecular orbital of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-COMO1.png|left|thumb|Picture1. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture1: This is the bonding orbital (3σ) formed by the overlap of two 2s orbital of carbon and oxygen atom, its energy is -1.15791 a.u.&lt;br /&gt;
[[File:01554120-COMO2.png|left|thumb|Picture1. The 4th orbital of ammonium ion ]]&lt;br /&gt;
Picture2: This is the 4σ orbital of the molecule, it is made by two head to head 2p orbitals overlap in phase. Its energy is -0.57004a.u. &lt;br /&gt;
[[File:01554120-COMO3.png|left|thumb|Picture1. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This is one of the degenerated 1π orbitals of the molecule, it is formed by two 2p orbital of each atom in phase parallel overlap and its energy is -0.46743 a.u. &lt;br /&gt;
[[File:01554120-COMO4.png|left|thumb|Picture1. The 7th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the 5σ orbital of the molecule, it is also the HOMO (energy=-0.37145). it is made by two out of phase 2s orbital from each atom overlap. &lt;br /&gt;
[[File:01554120-COMO5.png|left|thumb|Picture1. The 8th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is one of the degenerated 2π orbital of the molecule, it is also the LUMO (energy=-0.2177 a.u.). it is made by two out of phase 2p from each atom orbital parallel overlap.&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752258</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752258"/>
		<updated>2019-03-08T16:06:26Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: /* Analysis of CO molecule */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
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 &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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.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;
The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
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| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
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&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
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=Hydrogen molecule analysis=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -1.15928020 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 0.60±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&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 &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; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.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;
The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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=Transition metal complex=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
|-&lt;br /&gt;
| N-N bond length || 1.112Å&lt;br /&gt;
|-&lt;br /&gt;
| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
&lt;br /&gt;
Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
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=reaction energy of Haber-Bosch Process=&lt;br /&gt;
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&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
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=Analysis of ammonium ion=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
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| point group|| C1&lt;br /&gt;
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| bond length|| 1.03±0.01Å&lt;br /&gt;
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| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibrational modes for ammonium ion. &lt;br /&gt;
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[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
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| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
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| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
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Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-NH4-orb1.png|left|thumb|Picture1. The lowest orbital of ammonium ion ]]&lt;br /&gt;
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Picture1: This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. &lt;br /&gt;
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[[File:01554120-NH4-orb2.png|left|thumb|Picture2. The 2nd orbital of ammonium ion ]]&lt;br /&gt;
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Picture2: This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. &lt;br /&gt;
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[[File:01554120-NH4-orb3.png|left|thumb|Picture3. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This one of the bonding orbitals of ammonium ion, it is form by a nitrogen 2p orbital over with a hydrogen AO, &lt;br /&gt;
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[[File:01554120-NH4-orb5.png|left|thumb|Picture4. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the HOMO of the ammonium ion, it is the anti-bonding orbital of the overlap between 2s orbital of nitrogen and one of the four hydrogen atomic orbitals. Due to stablisation, the HOMO is quite close in energy (-0.82457 a.u.) with the previous 2 orbitals, not like the HOMO of ammonium molecule. &lt;br /&gt;
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[[File:01554120-NH4-orb6.png|left|thumb|Picture5. The 6th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is the LUMO of the ammonium ion, its energy (-0.20998 a.u.)is higher than the previous three molecular orbitals (approx-0.825 a.u.). and it is made from a p orbital of nitrogen and one of the four 4H atomic orbitals.&lt;br /&gt;
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=Analysis of CO molecule=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
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| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&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; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.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;
The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;Spectroscopy analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-CO-vib.png|thumb|left|spectroscopic data of carbon monoxide molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2209 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 67 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[01554120-CO-VM.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-CO-charge.png|200px|thumb|Atomic charge data of carbon monoxide molecule.]]&lt;br /&gt;
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&amp;lt;b&amp;gt;molecular orbital of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-COMO1.png|left|thumb|Picture1. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture1: This is the bonding orbital (3σ) formed by the overlap of two 2s orbital of carbon and oxygen atom, its energy is -1.15791 a.u.&lt;br /&gt;
[[File:01554120-COMO2.png|left|thumb|Picture1. The 4th orbital of ammonium ion ]]&lt;br /&gt;
Picture2: This is the 4σ orbital of the molecule, it is made by two head to head 2p orbitals overlap in phase. Its energy is -0.57004a.u. &lt;br /&gt;
[[File:01554120-COMO3.png|left|thumb|Picture1. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This is one of the degenerated 1π orbitals of the molecule, it is formed by two 2p orbital of each atom in phase parallel overlap and its energy is -0.46743 a.u. &lt;br /&gt;
[[File:01554120-COMO4.png|left|thumb|Picture1. The 7th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the 5σ orbital of the molecule, it is also the HOMO (energy=-0.37145). it is made by two out of phase 2s orbital from each atom overlap. &lt;br /&gt;
[[File:01554120-COMO5.png|left|thumb|Picture1. The 8th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is one of the degenerated 2π orbital of the molecule, it is also the LUMO (energy=-0.2177 a.u.). it is made by two out of phase 2p from each atom orbital parallel overlap.&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752256</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752256"/>
		<updated>2019-03-08T16:04:08Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
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 &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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&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; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.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;
The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
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&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
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=Hydrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
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| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
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| final energy|| -1.15928020 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
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| bond length|| 0.60±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&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 &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; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.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;
The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
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| calculation method || RB3LYP &lt;br /&gt;
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| basis set|| 6-31G(d,p)&lt;br /&gt;
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| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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=Transition metal complex=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
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| N-N bond length || 1.112Å&lt;br /&gt;
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| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
&lt;br /&gt;
Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
&lt;br /&gt;
=reaction energy of Haber-Bosch Process=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
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=Analysis of ammonium ion=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C1&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.03±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.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;
The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibrational modes for ammonium ion. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb1.png|left|thumb|Picture1. The lowest orbital of ammonium ion ]]&lt;br /&gt;
&lt;br /&gt;
Picture1: This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb2.png|left|thumb|Picture2. The 2nd orbital of ammonium ion ]]&lt;br /&gt;
&lt;br /&gt;
Picture2: This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb3.png|left|thumb|Picture3. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This one of the bonding orbitals of ammonium ion, it is form by a nitrogen 2p orbital over with a hydrogen AO, &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb5.png|left|thumb|Picture4. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the HOMO of the ammonium ion, it is the anti-bonding orbital of the overlap between 2s orbital of nitrogen and one of the four hydrogen atomic orbitals. Due to stablisation, the HOMO is quite close in energy (-0.82457 a.u.) with the previous 2 orbitals, not like the HOMO of ammonium molecule. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb6.png|left|thumb|Picture5. The 6th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is the LUMO of the ammonium ion, its energy (-0.20998 a.u.)is higher than the previous three molecular orbitals (approx-0.825 a.u.). and it is made from a p orbital of nitrogen and one of the four 4H atomic orbitals.&lt;br /&gt;
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=Analysis of CO molecule=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&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; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.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;
The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;b&amp;gt;Spectroscopy analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
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[[File:01554120-CO-vib.png|thumb|left|spectroscopic data of carbon monoxide molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2209 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 67 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[01554120-CO-VM.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-CO-charge.png|200px|thumb|Atomic charge data of carbon monoxide molecule.]]&lt;br /&gt;
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&amp;lt;b&amp;gt;molecular orbital of carbon monoxide&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-COMO1.png|left|thumb|Picture1. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
This is the bonding orbital (3σ) formed by the overlap of two 2s orbital of carbon and oxygen atom, its energy is -1.15791 a.u.&lt;br /&gt;
[[File:01554120-COMO2.png|left|thumb|Picture1. The 4th orbital of ammonium ion ]]&lt;br /&gt;
This is the 4σ orbital of the molecule, it is made by two head to head 2p orbitals overlap in phase. Its energy is -0.57004a.u. &lt;br /&gt;
[[File:01554120-COMO3.png|left|thumb|Picture1. The 5th orbital of ammonium ion ]]&lt;br /&gt;
This is one of the degenerated 1π orbitals of the molecule, it is formed by two 2p orbital of each atom in phase parallel overlap and its energy is -0.46743 a.u. &lt;br /&gt;
[[File:01554120-COMO4.png|left|thumb|Picture1. The 7th orbital of ammonium ion ]]&lt;br /&gt;
This is the 5σ orbital of the molecule, it is also the HOMO (energy=-0.37145). it is made by two out of phase 2s orbital from each atom overlap. &lt;br /&gt;
[[File:01554120-COMO5.png|left|thumb|Picture1. The 8th orbital of ammonium ion ]]&lt;br /&gt;
This is one of the degenerated 2π orbital of the molecule, it is also the LUMO (energy=-0.2177 a.u.). it is made by two out of phase 2p from each atom orbital parallel overlap.&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-COMO5.png&amp;diff=752249</id>
		<title>File:01554120-COMO5.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-COMO5.png&amp;diff=752249"/>
		<updated>2019-03-08T15:40:01Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-COMO4.png&amp;diff=752248</id>
		<title>File:01554120-COMO4.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-COMO4.png&amp;diff=752248"/>
		<updated>2019-03-08T15:39:49Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
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		<author><name>Jz13018</name></author>
	</entry>
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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-COMO3.png&amp;diff=752247</id>
		<title>File:01554120-COMO3.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-COMO3.png&amp;diff=752247"/>
		<updated>2019-03-08T15:39:35Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-COMO2.png&amp;diff=752246</id>
		<title>File:01554120-COMO2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-COMO2.png&amp;diff=752246"/>
		<updated>2019-03-08T15:39:23Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
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		<author><name>Jz13018</name></author>
	</entry>
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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-COMO1.png&amp;diff=752245</id>
		<title>File:01554120-COMO1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-COMO1.png&amp;diff=752245"/>
		<updated>2019-03-08T15:39:10Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
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		<author><name>Jz13018</name></author>
	</entry>
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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-CO-VM.png&amp;diff=752243</id>
		<title>File:01554120-CO-VM.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-CO-VM.png&amp;diff=752243"/>
		<updated>2019-03-08T15:24:49Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
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		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-CO-vib.png&amp;diff=752242</id>
		<title>File:01554120-CO-vib.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-CO-vib.png&amp;diff=752242"/>
		<updated>2019-03-08T15:24:25Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
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	</entry>
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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-CO-charge.png&amp;diff=752241</id>
		<title>File:01554120-CO-charge.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-CO-charge.png&amp;diff=752241"/>
		<updated>2019-03-08T15:22:12Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
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	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752240</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752240"/>
		<updated>2019-03-08T15:17:35Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: /* Analysis of ammonium ion */&lt;/p&gt;
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&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
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 &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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.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;
The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
&lt;br /&gt;
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=Hydrogen molecule analysis=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -1.15928020 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 0.60±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&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 &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; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.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;
The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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=Transition metal complex=&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
|-&lt;br /&gt;
| N-N bond length || 1.112Å&lt;br /&gt;
|-&lt;br /&gt;
| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
&lt;br /&gt;
Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
&lt;br /&gt;
=reaction energy of Haber-Bosch Process=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
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=Analysis of ammonium ion=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C1&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.03±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.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;
The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibrational modes for ammonium ion. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb1.png|left|thumb|Picture1. The lowest orbital of ammonium ion ]]&lt;br /&gt;
&lt;br /&gt;
Picture1: This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb2.png|left|thumb|Picture2. The 2nd orbital of ammonium ion ]]&lt;br /&gt;
&lt;br /&gt;
Picture2: This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb3.png|left|thumb|Picture3. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
Picture3: This one of the bonding orbitals of ammonium ion, it is form by a nitrogen 2p orbital over with a hydrogen AO, &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb5.png|left|thumb|Picture4. The 5th orbital of ammonium ion ]]&lt;br /&gt;
Picture4: This is the HOMO of the ammonium ion, it is the anti-bonding orbital of the overlap between 2s orbital of nitrogen and one of the four hydrogen atomic orbitals. Due to stablisation, the HOMO is quite close in energy (-0.82457 a.u.) with the previous 2 orbitals, not like the HOMO of ammonium molecule. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb6.png|left|thumb|Picture5. The 6th orbital of ammonium ion ]]&lt;br /&gt;
Picture5: This is the LUMO of the ammonium ion, its energy (-0.20998 a.u.)is higher than the previous three molecular orbitals (approx-0.825 a.u.). and it is made from a p orbital of nitrogen and one of the four 4H atomic orbitals.&lt;br /&gt;
&lt;br /&gt;
=Analysis of CO molecule=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&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; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.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;
The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752157</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752157"/>
		<updated>2019-03-08T13:57:10Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
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 &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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.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;
The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=Hydrogen molecule analysis=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -1.15928020 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 0.60±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&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 &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; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.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;
The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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=Transition metal complex=&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
|-&lt;br /&gt;
| N-N bond length || 1.112Å&lt;br /&gt;
|-&lt;br /&gt;
| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
&lt;br /&gt;
Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
&lt;br /&gt;
=reaction energy of Haber-Bosch Process=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
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=Analysis of ammonium ion=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C1&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.03±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.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;
The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibrational modes for ammonium ion. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb1.png|left|thumb|Picture1. The lowest orbital of ammonium ion ]]&lt;br /&gt;
&lt;br /&gt;
This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb2.png|left|thumb|Picture2. The 2nd orbital of ammonium ion ]]&lt;br /&gt;
&lt;br /&gt;
This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb3.png|left|thumb|Picture3. The 3rd orbital of ammonium ion ]]&lt;br /&gt;
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=Analysis of CO molecule=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.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;
The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752151</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752151"/>
		<updated>2019-03-08T13:53:24Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
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 &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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&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; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.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;
The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
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| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
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=Hydrogen molecule analysis=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -1.15928020 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 0.60±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
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&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 &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; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.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;
The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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=Transition metal complex=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
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| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
|-&lt;br /&gt;
| N-N bond length || 1.112Å&lt;br /&gt;
|-&lt;br /&gt;
| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
&lt;br /&gt;
Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
&lt;br /&gt;
=reaction energy of Haber-Bosch Process=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
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=Analysis of ammonium ion=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C1&lt;br /&gt;
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| bond length|| 1.03±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
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&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibrational modes for ammonium ion. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
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|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
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[[File:01554120-NH4-orb1.png|left|thumb|The lowest orbital of ammonium ion ]]&lt;br /&gt;
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This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. &lt;br /&gt;
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[[File:01554120-NH4-orb2.png|left|thumb|The lowest orbital of ammonium ion ]]&lt;br /&gt;
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This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. &lt;br /&gt;
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[[File:01554120-NH4-orb3.png|left|thumb|The lowest orbital of ammonium ion ]]&lt;br /&gt;
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=Analysis of CO molecule=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&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; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.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;
The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752143</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752143"/>
		<updated>2019-03-08T13:51:44Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: /* Analysis of ammonium ion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&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; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.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;
The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
&lt;br /&gt;
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=Hydrogen molecule analysis=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -1.15928020 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 0.60±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
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&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 &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; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.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;
The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
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=Nitrogen molecule analysis=&lt;br /&gt;
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{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
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=Transition metal complex=&lt;br /&gt;
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&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
|-&lt;br /&gt;
| N-N bond length || 1.112Å&lt;br /&gt;
|-&lt;br /&gt;
| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
&lt;br /&gt;
Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
&lt;br /&gt;
=reaction energy of Haber-Bosch Process=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
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=Analysis of ammonium ion=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C1&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.03±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
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&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
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The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
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&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibrational modes for ammonium ion. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
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&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb1.png|left|thumb|The lowest orbital of ammonium ion ]]&lt;br /&gt;
&lt;br /&gt;
This is the lowest energy orbital of NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+ ion, it is surrounded to the nitrogen atom, means it is the 1s orbital of nitrogen atom, its energy is very low (-14.71523 a.u.) so it cannot be included in bounding. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb2.png|left|thumb|The lowest orbital of ammonium ion ]]&lt;br /&gt;
&lt;br /&gt;
This is the second lowest energy orbital (-1.24818 a.u.). The AOs contributed to it are the 2s orbital of nitrogen and the mixed orbital from the 4 1s orbitals of the four hydrogen atoms.This orbital is the bonding orbital of the overlapping. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-orb3.png|left|thumb|The lowest orbital of ammonium ion ]]&lt;br /&gt;
&lt;br /&gt;
=Analysis of CO molecule=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&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; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.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;
The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-NH4-orb6.png&amp;diff=752123</id>
		<title>File:01554120-NH4-orb6.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-NH4-orb6.png&amp;diff=752123"/>
		<updated>2019-03-08T13:35:15Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-NH4-orb5.png&amp;diff=752122</id>
		<title>File:01554120-NH4-orb5.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-NH4-orb5.png&amp;diff=752122"/>
		<updated>2019-03-08T13:35:06Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-NH4-orb4.png&amp;diff=752121</id>
		<title>File:01554120-NH4-orb4.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-NH4-orb4.png&amp;diff=752121"/>
		<updated>2019-03-08T13:34:55Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-NH4-orb3.png&amp;diff=752120</id>
		<title>File:01554120-NH4-orb3.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-NH4-orb3.png&amp;diff=752120"/>
		<updated>2019-03-08T13:34:44Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-NH4-orb2.png&amp;diff=752119</id>
		<title>File:01554120-NH4-orb2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-NH4-orb2.png&amp;diff=752119"/>
		<updated>2019-03-08T13:34:31Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-NH4-orb1.png&amp;diff=752118</id>
		<title>File:01554120-NH4-orb1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:01554120-NH4-orb1.png&amp;diff=752118"/>
		<updated>2019-03-08T13:34:19Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752095</id>
		<title>Rep:Mod:JZ01554120</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Mod:JZ01554120&amp;diff=752095"/>
		<updated>2019-03-08T13:14:51Z</updated>

		<summary type="html">&lt;p&gt;Jz13018: /* Analysis of ammonium ion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=1. Ammonia molecules analysis=&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.55776873 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;V&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.02±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 106±1°&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&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     0.000070     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000033     0.001200     YES      &amp;lt;/pre&amp;gt;&lt;br /&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; ammonia 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JIAWEI ZHANG_01554120_PHUNT_NH3_OPTMF_POP.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;
The optimisation file is liked to [[Media:JIAWEI_ZHANG_01554120_PHUNT_NH3_OPTMF_POP.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-Screenshot.png|thumb|left|spectroscopic data of ammonia molecule.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1090 || 1694 || 1694 || 3461 || 3590 || 3590&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A1 || E || E || A1 || E || E&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 145 || 14 || 14 || 1 || 0 || 0&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120_vib1.png|150px]] || [[File:01554120_vib2.png|150px]] || [[File:01554120_vib3.png|150px]] || [[File:01554120_vib4.png|150px]] || [[File:01554120_vib5.png|150px]] || [[File:01554120_vib6.png|150px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
There are six expected modes of ammonia molecule according to the 3N-6 rule and four modes are degenerated ( two-two each). According to the table above, mode 3 and 4 are a pair of degenerated modes and mode 5 and 6 are another pair as they have same wavenumbers. The first three modes are all bending vibrations and last three are stretching vibrations. Mode 1 and 4 are highly symmetry, as they include point group A1, the other four modes only have E (identity). Mode 4 is called the umbrella mode. four brands are expected to see in a spectrum.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Atomic  charge of ammonia molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-ammonia-charge.png|left|200px]]&lt;br /&gt;
The charge of nitrogen atom is -1.125 and for each hydrogen atom is 0.375. The charges are expected to be 0.230 (positive) for hydrogen and -0.690 (negative) for nitrogen from calculation through dipole moment, and because nitrogen is more electronegative compare with hydrogen, it is expected to carry the negative charge.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=Hydrogen molecule analysis=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -1.15928020 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 0.60±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&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 &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; hydrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_HYDROGEN_MOLECULE_OPT.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;
The optimisation file is liked to [[Media:01554120_HYDROGEN_MOLECULE_OPT.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopic properties&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-h2-vib.png|thumb|left|spectroscopic data of hydrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 4466 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-h2-vib-mode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
3N-5 rule is applied here as hydrogen is a linear molecule, and only one vibration mode of stretching vibration is expected to see. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Charge of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule&amp;lt;/b&amp;gt;&lt;br /&gt;
[[File:01554120-h2-charge.png|200px|thumb|left|Atomic charge data of hydrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
Atomic charge of hydrogen is 0 as it is a uniatomic molecule and the two H atoms have same electronegativity.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=Nitrogen molecule analysis=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -109.52359111 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| D∞h&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.09±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;            Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; nitrogen 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;01554120_NITROGEN_MOLECULE_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;
The optimisation file is liked to [[Media:01554120_NITROGEN_MOLECULE_OPTIMISATION.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Spectroscopic analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-vib.png|thumb|left|spectroscopic data of nitrogen molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 &lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 2457 &lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || SGG &lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 0 &lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-n2-vibmode.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Charge analysis of nitrogen&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-n2-charge.png|200px|thumb|left|Atomic charge data of hydrogen 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;
&lt;br /&gt;
&lt;br /&gt;
=Transition metal complex=&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Name|| (dinitrogen)-(2,6-bis(1-(2,6-diisopropylphenylimino)propyl)pyridine)-iron&lt;br /&gt;
|-&lt;br /&gt;
| Code|| BARTOF&lt;br /&gt;
|-&lt;br /&gt;
| N-N bond length || 1.112Å&lt;br /&gt;
|-&lt;br /&gt;
| image||[[File:01554120-TMCPLX.png|500px]]&lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The structure can be found [[https://www.ccdc.cam.ac.uk/structures/Search?Ccdcid=BARTOF&amp;amp;DatabaseToSearch=Published   here]]&lt;br /&gt;
&lt;br /&gt;
Bond length between the two nitrogen atom is longer compare with the N-N bond in nitrogen molecule. This is because when the nitrogen molecule bonded with a electron rich transition element like Fe, electron density is pushed into the anti-bonding π* orbital and weaken the N-N bond. therefore, the bond length of N-N bond will increase when it for complex ions. it also because the electron density becomes diffused when a new bond is formed between nitrogen molecule and a metal atom. &lt;br /&gt;
In this situation, as the value is obtained from computational calculation, there may also be certain degree of inaccuracy. &lt;br /&gt;
&lt;br /&gt;
=reaction energy of Haber-Bosch Process=&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;E(NH3)=-56.5577687&lt;br /&gt;
2*E(NH3)=-113.1155374&lt;br /&gt;
E(N2)=-109.5235911&lt;br /&gt;
E(H2)=-1.1592802&lt;br /&gt;
3*E(H2)=-3.4778406&lt;br /&gt;
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-113.1155374-[-109.5235911-3.4778406]=-0.1141057&lt;br /&gt;
ΔE=2625.5*-0.1141057=-299.6kjmol-1&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=Analysis of ammonium ion=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| NH&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;+&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -56.89738175 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C1&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.03±0.01Å&lt;br /&gt;
|-&lt;br /&gt;
| bond angle|| 109±1°&lt;br /&gt;
|}&lt;br /&gt;
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&amp;lt;pre&amp;gt;         Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000203     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000097     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.001016     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000578     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&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; ammonium ion &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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;JZ-NH4-OPT.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;
The optimisation file is liked to [[Media:JZ-NH4-OPT.LOG| here]]&lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;spectroscopy analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
According to the 3N-6 rule, there are 9 vibrational modes for ammonium ion. &lt;br /&gt;
&lt;br /&gt;
[[File:01554120-NH4-Spectroscopy.png|thumb|left|spectroscopic data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| Models|| 1 || 2 || 3 || 4 || 5 || 6 || 7 || 8 || 9&lt;br /&gt;
|-&lt;br /&gt;
| wavenumber/cm-1|| 1495 || 1496 || 1497 || 1726 || 1727 || 3368 || 3491 || 3493 || 3495&lt;br /&gt;
|-&lt;br /&gt;
| Symmetry || A || A || A || A || A || A || A || A || A&lt;br /&gt;
|-&lt;br /&gt;
| intensity/arbitrary units|| 181 || 181 || 181 || 0 || 0 || 0 || 197 || 198 || 198&lt;br /&gt;
|-&lt;br /&gt;
| image|| [[File:01554120-NH4-VibM1.png|150px]] || [[File:01554120-NH4-VibM2.png|150px]] || [[File:01554120-NH4-VibM3.png|150px]] || [[File:01554120-NH4-VibM4.png|150px]] || [[File:01554120-NH4-VibM5.png|150px]] || [[File:01554120-NH4-VibM6.png|150px]] || [[File:01554120-NH4-VibM7.png|150px]] || [[File:01554120-NH4-VibM8.png|150px]] || [[File:01554120-NH4-VibM9.png|150px]] &lt;br /&gt;
|- &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Charge analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:01554120-AmmoniumCharge.png|thumb|left|charge data of ammonium molecule.]]&lt;br /&gt;
&lt;br /&gt;
Nitrogen atom bare negative charge and hydrogen atoms bear positive charge, this is because the electronegativity of nitrogen is bigger than hydrogen. The overall charge is not 0 as the ion is not a neutral species and it has +1 overall charge. &lt;br /&gt;
&lt;br /&gt;
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&lt;br /&gt;
&amp;lt;b&amp;gt;Molecular orbital analysis of ammonium ion&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=Analysis of CO molecule=&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
&lt;br /&gt;
|-&lt;br /&gt;
| molecule name|| CO&lt;br /&gt;
|-&lt;br /&gt;
| calculation method || RB3LYP &lt;br /&gt;
|-&lt;br /&gt;
| basis set|| 6-31G(d,p)&lt;br /&gt;
|-&lt;br /&gt;
| final energy|| -113.30945314 a.u.&lt;br /&gt;
|-&lt;br /&gt;
| point group|| C∞v&lt;br /&gt;
|-&lt;br /&gt;
| bond length|| 1.14±0.01Å&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;     Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000032     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000032     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000018     0.001200     YES&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; carbon monoxide 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;350&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;CO-OPT-01554120-NEW.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;
The optimisation file is liked to [[Media:CO-OPT-01554120-NEW.LOG| here]]&lt;/div&gt;</summary>
		<author><name>Jz13018</name></author>
	</entry>
</feed>