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	<updated>2026-06-16T22:13:22Z</updated>
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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Jr407:portal&amp;diff=86139</id>
		<title>Rep:Jr407:portal</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Jr407:portal&amp;diff=86139"/>
		<updated>2009-12-30T10:12:31Z</updated>

		<summary type="html">&lt;p&gt;Jr407: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:Chemistry.jpg|thumb|left|200px|]]&lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;jr407 - Computational Chemistry Lab (3rd. yr.)&#039;&#039;&#039;=&lt;br /&gt;
&lt;br /&gt;
===Pages===&lt;br /&gt;
* [Module 1: Organic https://www.ch.imperial.ac.uk/wiki/index.php/Namespace:jr407]&lt;br /&gt;
* [Module 2: Inorganic https://www.ch.imperial.ac.uk/wiki/index.php/Namespace:jr4072]&lt;br /&gt;
* [Module 2 Mini-Project: https://www.ch.imperial.ac.uk/wiki/index.php/Namespace:jr4072PROJECT]&lt;br /&gt;
* [Module 3: Physical https://www.ch.imperial.ac.uk/wiki/index.php/Namespace:jr4073]&lt;br /&gt;
* [Module 3 Mini-Project: https://www.ch.imperial.ac.uk/wiki/index.php/Namespace:jr4073PROJECT]&lt;br /&gt;
&lt;br /&gt;
===External Links===&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Jr407:portal&amp;diff=86138</id>
		<title>Rep:Jr407:portal</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Jr407:portal&amp;diff=86138"/>
		<updated>2009-12-30T10:05:35Z</updated>

		<summary type="html">&lt;p&gt;Jr407: New page: Hello&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Hello&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85579</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85579"/>
		<updated>2009-12-18T11:43:07Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result, and semi-empirical (AM1) calculations to show MOs.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
[[Image:jr407methylenemos.jpg|thumb|right|Ethylene MOs]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right). The optimised molecule is fully planar with a dihedral angle of 0deg (C-C-C-C).&lt;br /&gt;
&lt;br /&gt;
The MOs of ethylene have also been computed in the same manner (shown right), the HOMO being symmetric and the LUMO anti-symmetric this time though, with no nodal planes in the HOMO and one in the LUMO.&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; bonded carbon has a C-C bondlength of 1.54Å, and sp&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
Notably the LUMO of the transition state is formed by the combination of the ethylene HOMO and cis-butadiene LUMO (both symmetric, s); the ethylene HOMO and LUMO are of course the pi and pi* bonding and anti-bonding MOs. The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Like the reaction of ethylene and cis-butadiene, the reaction is likely to proceed via donation from the HOMO of the diene to the LUMO of the dieneophile (maleic anhydride); this is further enhanced by the electron withdrawing substituents on the diene, creating a dipole to pull electron density towards itself. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|400 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details).&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Main Page: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073]&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073&amp;diff=85561</id>
		<title>Rep:Namespace:jr4073</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073&amp;diff=85561"/>
		<updated>2009-12-18T11:22:07Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Higher level optimisation to determine activation energies &amp;amp; discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstates.jpg|thumb|left|200px|Transition State Theory (Michigan Engineering College)]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Computational Chemistry - Introduction and application...&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Computational chemistry allows us to model transition states and potential energy surfaces to predict reactivity, which has many applications, illustrated here with the Cope rearrangement and Diels Alder cycloaddition reactions.  &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;Computational Chemistry - Module 3: Physical&#039;&#039;&#039;=&lt;br /&gt;
The first section of this investigation illustrates the virtues of computational methods in determining transition states, using the Cope Rearrangement as an example. The mini-project that follows then applies these methods to deduce new conclusions. &lt;br /&gt;
&lt;br /&gt;
==Cope Rearrangement==&lt;br /&gt;
[[Image:jr407m3p1cope.jpg|thumb|right|The Cope rearrangement.]]&lt;br /&gt;
&lt;br /&gt;
Computational methods are used to investigate transition states (potential energy minima) for the Cope rearrangement of 1,5-hexadiene to determine the preferred mechanism (step-wise, dissociative or concerted). This is begun with a conformational analysis of the reactants before considering transition state geometry (chair or boat). &lt;br /&gt;
&lt;br /&gt;
===Conformational analysis of hexadiene===&lt;br /&gt;
[[Image:jr407m3p1apph.jpg|thumb|right|Anti Hexadiene- click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Jr407Hexadienejmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Anti Hexadiene3D - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3p1gaucheh.jpg|thumb|right|Gauche Hexadiene - click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Hexadienechemgauchejmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Gauche Hexadiene - 3D JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3p1anti2dft.jpg|thumb|right|Anti2 conformation (hexadiene).]]&lt;br /&gt;
[[Image:jr407m3p1anti2ir.jpg|thumb|right|IR spectra (anti2 hexadiene).]]&lt;br /&gt;
&lt;br /&gt;
Molecules may exist in various conformations, of differing energies. For substituted carbons these may be termed depending upon the arrangement of substituents relative to each other, this is illustrated below by Newman projection.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforexam.jpg|center|800 x 300 px|thumb|Conformational analysis: butane in example.]]&lt;br /&gt;
&lt;br /&gt;
1,5-hexadiene has been geometry optimised in Gaussian (method: Hartree-Fock [HF]; basis set: 3-21G) for both the anti and gauche conformation (of the central four C atoms); the %mem term has been set at 250MB and 500MB for both calculations, showing no difference in the results. The energy and symmetry (point group) of the optimised structures are tabulated below. One would expect the gauche conformation to be at a higher energy, and this is the initial result. However, a number of possible gauche structures can be imagined, and these have also been optimised, identifying a gauche conformation at lower energy than the anti, which match the reference structures (https://www.ch.ic.ac.uk/wiki/index.php/Mod:phys3#Appendix_1). This is a result of the gauche conformer increasing the entropy of the system, which is favourable.&lt;br /&gt;
&lt;br /&gt;
The initial anti and gauche conformations are shown right (click to enlarge; links to 3D JMols).&lt;br /&gt;
&lt;br /&gt;
*Note: the numbering of gauche conformations in the table below does not intend to correspond with the numbering on the reference table &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforsresults.jpg|center|800 x 300 px|thumb|Conformations of hexadiene.]]&lt;br /&gt;
&lt;br /&gt;
A further anti conformation has been modelled also, shown right. The Ci (symmetry) anti2 conformation of 1,5-hexadiene has been optimised at both the HF/3-21G and B3LYP/6-31G* level, the energies are tabulated below. There is essentially no difference between the geometry of the two structures, but a large difference in energy. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforsresults2.jpg|center|300 x 150 px|thumb|Anti conformations of hexadiene: differing basis sets.]]&lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the structures to be minimal energy (vibrational frequecies are the second derivative of energy, being real and positive thus corresponds to a minima point). For the higher level calculation, the &#039;low frequencies&#039; are:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---   -9.4888   -0.0006   -0.0006    0.0002    3.7552   13.0176&lt;br /&gt;
 Low frequencies ---   74.2853   80.9980  121.4178&lt;br /&gt;
&lt;br /&gt;
The infrared spectrum is shown right. The vibrational analysis also computes real properties that may be compared:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=           -234.469204&lt;br /&gt;
 Sum of electronic and thermal Energies=              -234.461857&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=            -234.460913&lt;br /&gt;
 Sum of electronic and thermal Free Energies=         -234.500777&lt;br /&gt;
&lt;br /&gt;
The first of these is the potential energy at 0 K including the zero-point vibrational energy (E = Eelec + ZPE), the second is the energy at 298.15 K and 1 atm of pressure which includes contributions from the translational, rotational, and vibrational energy modes at this temperature (E = E + Evib + Erot + Etrans), the third contains an additional correction for RT (H = E + RT) which is particularly important when looking at dissociation reactions, and the last includes the entropic contribution to the free energy (G = H - TS).&lt;br /&gt;
&lt;br /&gt;
===Optimising the chair and boat transition structures===&lt;br /&gt;
[[Image:jr407m3p2conforms.jpg|right|200 x 200 px|thumb|The conformations of cyclohexane (http://wps.prenhall.com/wps/media/objects/724/741576/).]]&lt;br /&gt;
[[Image:jr407m3p2conformchair.jpg|right|200 x 200 px|thumb|Modelling the chair transition state.]]&lt;br /&gt;
The chair and boat conformations of cyclohexane are illustrated right (also showing their relative energies), as transition states the atoms are in these arrangements with bond being made and broken.  &lt;br /&gt;
&lt;br /&gt;
====Optimisation to a TS (Berny; chair)====&lt;br /&gt;
Initially the delocalised allyl fragment (CH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;CHCH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) was optimised (HF/3-21G) and configured in the assumed chair transition state (terminal C&#039;s approx. 2.2a.u. apart): this is shown right. A vibrational analysis was performed, revealing an imaginary vibration at 818cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; corresponding to the Cope rearrangement - this is shown below; the optimised transition state structure is shown right, with a distance of 2.02a.u. between the terminal carbons of each fragment.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p2chairir.jpg|center|400 x 200 px|thumb|Vibrational analysis of chair transition state.]]&lt;br /&gt;
&lt;br /&gt;
====Frozen coordinate method (chair)====&lt;br /&gt;
The transition state optimisation was repeated with frozen coordinates (the bond distance between the terminal carbons fixed), this was then repeated with the frozen coordinate bond as a derivative (no force constants calculated). The optimised lengths of the bond forming/breaking is retained at 2.02a.u. This corresponds to the chair transition state, with the same appearance as that of the TS (Berny) method, shown right.&lt;br /&gt;
&lt;br /&gt;
====QST2 method (boat)====&lt;br /&gt;
[[Image:jr407m3p2nunbersnumbers.jpg|right|200 x 200 px|thumb|Carbon numbering.]]&lt;br /&gt;
The boat transition state is optimised by the QST2 method: specifying the reactant and product structures, with the calculation interpolating between the two; crucial to this is a numbering of the carbons in the reactant and product that match. This method is not possible with the anti conformer of the reactant as rotation about the central bond is not possible and a transition state corresponds not to the Cope rearrangement. However, adjusting the reactant geometries allows for a boat transition state. This is illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p2confomersqst2.jpg|center|400 x 200 px|thumb|QST2 transition state determination.]]&lt;br /&gt;
&lt;br /&gt;
The bottom carbons of the fragments are separated &#039;through space&#039; by 2.14a.u., CC distances in the fragments 1.38a.u.; the further apart carbons at the top of each fragment are separated by 2.78a.u. through space.&lt;br /&gt;
&lt;br /&gt;
===Intermediate reaction coordinate analysis===&lt;br /&gt;
[[Image:jr407m3p4nomingra.jpg|right|200 x 200 px|thumb|Inititally a minima is not achieved.]]&lt;br /&gt;
&lt;br /&gt;
The optimised chair and boat transition structures connect conformers of 1,5-hexadiene, though by visual inspection it is nearly impossible to tell which ones. This is determined instead by following the minimum enery path from the transition state down to the local minimum (reactants) on a potential energy surface (intrinsic reaction coordinate [IRC] method in Gaussian). &lt;br /&gt;
&lt;br /&gt;
Force constants have been determined once at the beggining of the calculation, running the reaction coordinate in just the forward direction (since this is symmetrical), with 50 points. Initially a minimum is not reached (the gradient does not fall to zero - see graph, right), leaving three options:&lt;br /&gt;
*take the last point on the IRC and run a normal minimization (may lead to a local minima)&lt;br /&gt;
*restart the IRC and specify a larger number of points until it reaches a minimum (if not enough points, again a local minima)&lt;br /&gt;
*redo the IRC specifying to compute the force constants at every step (expensive and infeasible for large systems)&lt;br /&gt;
&lt;br /&gt;
The third option has been implemented, revealing the chair to result from conformer gauche 2 (see reference table: https://www.ch.ic.ac.uk/wiki/index.php/Mod:phys3) and the boat from a rather higher energy totally eclipsed conformer, resembling that used for the modified QST2 calculations above (a minimum was not achieved here, even using 100 iteration points). &lt;br /&gt;
&lt;br /&gt;
The reaction coordinate paths for the chair and boat transition states are illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p3chairirc.jpg|center|1000 x 500 px|thumb|IRC method: chair and boat transition states.]]&lt;br /&gt;
&lt;br /&gt;
===Higher level optimisation to determine activation energies &amp;amp; discussion===&lt;br /&gt;
[[Image:jr407m3p5631goptchair.jpg|thumb|right|6-31G* TS&#039;s.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Optchair631gJMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Chair TS (6-31G*) - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:Jr407m3p5631goptboat.jpg|thumb|right|Gauche Hexadiene - click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Optboat631gjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Boat TS (6-31G*) - 3D JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
The chair and boat transition structures have been reoptimised at the higher B3LYP/6-31G* level of theory, these are shown right with links to 3D JMols (note these return the structure to a localised bonding representation). The energies of the transition structures are both levels of theory are tabulated below and activation energies calculated, at the higher level of theory these are in fair aggreement with the experimental values (0K) when accounting for error, being no more than 1 kcal/mol out. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p5tableacen.jpg|center|800 x 300 px|thumb|Activation energies; note: 1 a.u. = 627.509 kcal/mol.]]&lt;br /&gt;
&lt;br /&gt;
A geometry analysis has also been performed, investigating the through space separation of the fragments in the transition state, and C-C bond lengths within the fragments at the different levels of theory. These are tabulated (and illustrated) below.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p5tabgeocompts.jpg|center|800 x 300 px|thumb|Geometric comparison of transition states.]]&lt;br /&gt;
&lt;br /&gt;
In summary the geometry changes minimally at the higher level of theory, while the molecules are greatly stabilised and found to have much lower energies (more accurate also, being a better agreement with experimental data for activation energy).&lt;br /&gt;
&lt;br /&gt;
It is concluded that under kinetic control the reaction will proceed via the chair transition state as this has the lower activation energy.&lt;br /&gt;
&lt;br /&gt;
==Mini-Project==&lt;br /&gt;
A mini-project in transition state computational chemistry has been conducted based on the Diels-Alder cycloaddition. &lt;br /&gt;
&lt;br /&gt;
The projects should be viewed here: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073PROJECT.&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details).&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan Engineering College - Transition State Theory: http://www.engin.umich.edu/]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;br /&gt;
* [Mini-project: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073PROJECT]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073&amp;diff=85558</id>
		<title>Rep:Namespace:jr4073</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073&amp;diff=85558"/>
		<updated>2009-12-18T11:21:03Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Higher level optimisation to determine activation energies */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstates.jpg|thumb|left|200px|Transition State Theory (Michigan Engineering College)]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Computational Chemistry - Introduction and application...&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Computational chemistry allows us to model transition states and potential energy surfaces to predict reactivity, which has many applications, illustrated here with the Cope rearrangement and Diels Alder cycloaddition reactions.  &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;Computational Chemistry - Module 3: Physical&#039;&#039;&#039;=&lt;br /&gt;
The first section of this investigation illustrates the virtues of computational methods in determining transition states, using the Cope Rearrangement as an example. The mini-project that follows then applies these methods to deduce new conclusions. &lt;br /&gt;
&lt;br /&gt;
==Cope Rearrangement==&lt;br /&gt;
[[Image:jr407m3p1cope.jpg|thumb|right|The Cope rearrangement.]]&lt;br /&gt;
&lt;br /&gt;
Computational methods are used to investigate transition states (potential energy minima) for the Cope rearrangement of 1,5-hexadiene to determine the preferred mechanism (step-wise, dissociative or concerted). This is begun with a conformational analysis of the reactants before considering transition state geometry (chair or boat). &lt;br /&gt;
&lt;br /&gt;
===Conformational analysis of hexadiene===&lt;br /&gt;
[[Image:jr407m3p1apph.jpg|thumb|right|Anti Hexadiene- click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Jr407Hexadienejmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Anti Hexadiene3D - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3p1gaucheh.jpg|thumb|right|Gauche Hexadiene - click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Hexadienechemgauchejmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Gauche Hexadiene - 3D JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3p1anti2dft.jpg|thumb|right|Anti2 conformation (hexadiene).]]&lt;br /&gt;
[[Image:jr407m3p1anti2ir.jpg|thumb|right|IR spectra (anti2 hexadiene).]]&lt;br /&gt;
&lt;br /&gt;
Molecules may exist in various conformations, of differing energies. For substituted carbons these may be termed depending upon the arrangement of substituents relative to each other, this is illustrated below by Newman projection.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforexam.jpg|center|800 x 300 px|thumb|Conformational analysis: butane in example.]]&lt;br /&gt;
&lt;br /&gt;
1,5-hexadiene has been geometry optimised in Gaussian (method: Hartree-Fock [HF]; basis set: 3-21G) for both the anti and gauche conformation (of the central four C atoms); the %mem term has been set at 250MB and 500MB for both calculations, showing no difference in the results. The energy and symmetry (point group) of the optimised structures are tabulated below. One would expect the gauche conformation to be at a higher energy, and this is the initial result. However, a number of possible gauche structures can be imagined, and these have also been optimised, identifying a gauche conformation at lower energy than the anti, which match the reference structures (https://www.ch.ic.ac.uk/wiki/index.php/Mod:phys3#Appendix_1). This is a result of the gauche conformer increasing the entropy of the system, which is favourable.&lt;br /&gt;
&lt;br /&gt;
The initial anti and gauche conformations are shown right (click to enlarge; links to 3D JMols).&lt;br /&gt;
&lt;br /&gt;
*Note: the numbering of gauche conformations in the table below does not intend to correspond with the numbering on the reference table &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforsresults.jpg|center|800 x 300 px|thumb|Conformations of hexadiene.]]&lt;br /&gt;
&lt;br /&gt;
A further anti conformation has been modelled also, shown right. The Ci (symmetry) anti2 conformation of 1,5-hexadiene has been optimised at both the HF/3-21G and B3LYP/6-31G* level, the energies are tabulated below. There is essentially no difference between the geometry of the two structures, but a large difference in energy. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforsresults2.jpg|center|300 x 150 px|thumb|Anti conformations of hexadiene: differing basis sets.]]&lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the structures to be minimal energy (vibrational frequecies are the second derivative of energy, being real and positive thus corresponds to a minima point). For the higher level calculation, the &#039;low frequencies&#039; are:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---   -9.4888   -0.0006   -0.0006    0.0002    3.7552   13.0176&lt;br /&gt;
 Low frequencies ---   74.2853   80.9980  121.4178&lt;br /&gt;
&lt;br /&gt;
The infrared spectrum is shown right. The vibrational analysis also computes real properties that may be compared:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=           -234.469204&lt;br /&gt;
 Sum of electronic and thermal Energies=              -234.461857&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=            -234.460913&lt;br /&gt;
 Sum of electronic and thermal Free Energies=         -234.500777&lt;br /&gt;
&lt;br /&gt;
The first of these is the potential energy at 0 K including the zero-point vibrational energy (E = Eelec + ZPE), the second is the energy at 298.15 K and 1 atm of pressure which includes contributions from the translational, rotational, and vibrational energy modes at this temperature (E = E + Evib + Erot + Etrans), the third contains an additional correction for RT (H = E + RT) which is particularly important when looking at dissociation reactions, and the last includes the entropic contribution to the free energy (G = H - TS).&lt;br /&gt;
&lt;br /&gt;
===Optimising the chair and boat transition structures===&lt;br /&gt;
[[Image:jr407m3p2conforms.jpg|right|200 x 200 px|thumb|The conformations of cyclohexane (http://wps.prenhall.com/wps/media/objects/724/741576/).]]&lt;br /&gt;
[[Image:jr407m3p2conformchair.jpg|right|200 x 200 px|thumb|Modelling the chair transition state.]]&lt;br /&gt;
The chair and boat conformations of cyclohexane are illustrated right (also showing their relative energies), as transition states the atoms are in these arrangements with bond being made and broken.  &lt;br /&gt;
&lt;br /&gt;
====Optimisation to a TS (Berny; chair)====&lt;br /&gt;
Initially the delocalised allyl fragment (CH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;CHCH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) was optimised (HF/3-21G) and configured in the assumed chair transition state (terminal C&#039;s approx. 2.2a.u. apart): this is shown right. A vibrational analysis was performed, revealing an imaginary vibration at 818cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; corresponding to the Cope rearrangement - this is shown below; the optimised transition state structure is shown right, with a distance of 2.02a.u. between the terminal carbons of each fragment.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p2chairir.jpg|center|400 x 200 px|thumb|Vibrational analysis of chair transition state.]]&lt;br /&gt;
&lt;br /&gt;
====Frozen coordinate method (chair)====&lt;br /&gt;
The transition state optimisation was repeated with frozen coordinates (the bond distance between the terminal carbons fixed), this was then repeated with the frozen coordinate bond as a derivative (no force constants calculated). The optimised lengths of the bond forming/breaking is retained at 2.02a.u. This corresponds to the chair transition state, with the same appearance as that of the TS (Berny) method, shown right.&lt;br /&gt;
&lt;br /&gt;
====QST2 method (boat)====&lt;br /&gt;
[[Image:jr407m3p2nunbersnumbers.jpg|right|200 x 200 px|thumb|Carbon numbering.]]&lt;br /&gt;
The boat transition state is optimised by the QST2 method: specifying the reactant and product structures, with the calculation interpolating between the two; crucial to this is a numbering of the carbons in the reactant and product that match. This method is not possible with the anti conformer of the reactant as rotation about the central bond is not possible and a transition state corresponds not to the Cope rearrangement. However, adjusting the reactant geometries allows for a boat transition state. This is illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p2confomersqst2.jpg|center|400 x 200 px|thumb|QST2 transition state determination.]]&lt;br /&gt;
&lt;br /&gt;
The bottom carbons of the fragments are separated &#039;through space&#039; by 2.14a.u., CC distances in the fragments 1.38a.u.; the further apart carbons at the top of each fragment are separated by 2.78a.u. through space.&lt;br /&gt;
&lt;br /&gt;
===Intermediate reaction coordinate analysis===&lt;br /&gt;
[[Image:jr407m3p4nomingra.jpg|right|200 x 200 px|thumb|Inititally a minima is not achieved.]]&lt;br /&gt;
&lt;br /&gt;
The optimised chair and boat transition structures connect conformers of 1,5-hexadiene, though by visual inspection it is nearly impossible to tell which ones. This is determined instead by following the minimum enery path from the transition state down to the local minimum (reactants) on a potential energy surface (intrinsic reaction coordinate [IRC] method in Gaussian). &lt;br /&gt;
&lt;br /&gt;
Force constants have been determined once at the beggining of the calculation, running the reaction coordinate in just the forward direction (since this is symmetrical), with 50 points. Initially a minimum is not reached (the gradient does not fall to zero - see graph, right), leaving three options:&lt;br /&gt;
*take the last point on the IRC and run a normal minimization (may lead to a local minima)&lt;br /&gt;
*restart the IRC and specify a larger number of points until it reaches a minimum (if not enough points, again a local minima)&lt;br /&gt;
*redo the IRC specifying to compute the force constants at every step (expensive and infeasible for large systems)&lt;br /&gt;
&lt;br /&gt;
The third option has been implemented, revealing the chair to result from conformer gauche 2 (see reference table: https://www.ch.ic.ac.uk/wiki/index.php/Mod:phys3) and the boat from a rather higher energy totally eclipsed conformer, resembling that used for the modified QST2 calculations above (a minimum was not achieved here, even using 100 iteration points). &lt;br /&gt;
&lt;br /&gt;
The reaction coordinate paths for the chair and boat transition states are illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p3chairirc.jpg|center|1000 x 500 px|thumb|IRC method: chair and boat transition states.]]&lt;br /&gt;
&lt;br /&gt;
===Higher level optimisation to determine activation energies &amp;amp; discussion===&lt;br /&gt;
[[Image:jr407m3p5631goptchair.jpg|thumb|right|6-31G* TS&#039;s.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Optchair631gJMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Chair TS (6-31G*) - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:Jr407m3p5631goptboat.jpg|thumb|right|Gauche Hexadiene - click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Optboat631gjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Boat TS (6-31G*) - 3D JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
The chair and boat transition structures have been reoptimised at the higher B3LYP/6-31G* level of theory, these are shown right with links to 3D JMols (note these return the structure to a localised bonding representation). The energies of the transition structures are both levels of theory are tabulated below and activation energies calculated, at the higher level of theory these are in fair aggreement with the experimental values (0K) when accounting for error, being no more than 1 kcal/mol out. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p5tableacen.jpg|center|800 x 300 px|thumb|Activation energies; note: 1 a.u. = 627.509 kcal/mol.]]&lt;br /&gt;
&lt;br /&gt;
A geometry analysis has also been performed, investigating the through space separation of the fragments in the transition state, and C-C bond lengths within the fragments at the different levels of theory. These are tabulated (and illustrated) below.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p5tabgeocompts.jpg|center|800 x 300 px|thumb|Geometric comparison of transition states.]]&lt;br /&gt;
&lt;br /&gt;
In summary the geometry changes minimally at the higher level of theory, while the molecules are greatly stabilised and found to have much lower energies (more accurate also, being a better agreement with experimental data for activation energy).&lt;br /&gt;
&lt;br /&gt;
==Mini-Project==&lt;br /&gt;
A mini-project in transition state computational chemistry has been conducted based on the Diels-Alder cycloaddition. &lt;br /&gt;
&lt;br /&gt;
The projects should be viewed here: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073PROJECT.&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details).&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan Engineering College - Transition State Theory: http://www.engin.umich.edu/]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;br /&gt;
* [Mini-project: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073PROJECT]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073&amp;diff=85553</id>
		<title>Rep:Namespace:jr4073</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073&amp;diff=85553"/>
		<updated>2009-12-18T11:17:17Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Conformational analysis of hexadiene */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstates.jpg|thumb|left|200px|Transition State Theory (Michigan Engineering College)]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Computational Chemistry - Introduction and application...&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Computational chemistry allows us to model transition states and potential energy surfaces to predict reactivity, which has many applications, illustrated here with the Cope rearrangement and Diels Alder cycloaddition reactions.  &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;Computational Chemistry - Module 3: Physical&#039;&#039;&#039;=&lt;br /&gt;
The first section of this investigation illustrates the virtues of computational methods in determining transition states, using the Cope Rearrangement as an example. The mini-project that follows then applies these methods to deduce new conclusions. &lt;br /&gt;
&lt;br /&gt;
==Cope Rearrangement==&lt;br /&gt;
[[Image:jr407m3p1cope.jpg|thumb|right|The Cope rearrangement.]]&lt;br /&gt;
&lt;br /&gt;
Computational methods are used to investigate transition states (potential energy minima) for the Cope rearrangement of 1,5-hexadiene to determine the preferred mechanism (step-wise, dissociative or concerted). This is begun with a conformational analysis of the reactants before considering transition state geometry (chair or boat). &lt;br /&gt;
&lt;br /&gt;
===Conformational analysis of hexadiene===&lt;br /&gt;
[[Image:jr407m3p1apph.jpg|thumb|right|Anti Hexadiene- click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Jr407Hexadienejmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Anti Hexadiene3D - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3p1gaucheh.jpg|thumb|right|Gauche Hexadiene - click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Hexadienechemgauchejmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Gauche Hexadiene - 3D JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3p1anti2dft.jpg|thumb|right|Anti2 conformation (hexadiene).]]&lt;br /&gt;
[[Image:jr407m3p1anti2ir.jpg|thumb|right|IR spectra (anti2 hexadiene).]]&lt;br /&gt;
&lt;br /&gt;
Molecules may exist in various conformations, of differing energies. For substituted carbons these may be termed depending upon the arrangement of substituents relative to each other, this is illustrated below by Newman projection.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforexam.jpg|center|800 x 300 px|thumb|Conformational analysis: butane in example.]]&lt;br /&gt;
&lt;br /&gt;
1,5-hexadiene has been geometry optimised in Gaussian (method: Hartree-Fock [HF]; basis set: 3-21G) for both the anti and gauche conformation (of the central four C atoms); the %mem term has been set at 250MB and 500MB for both calculations, showing no difference in the results. The energy and symmetry (point group) of the optimised structures are tabulated below. One would expect the gauche conformation to be at a higher energy, and this is the initial result. However, a number of possible gauche structures can be imagined, and these have also been optimised, identifying a gauche conformation at lower energy than the anti, which match the reference structures (https://www.ch.ic.ac.uk/wiki/index.php/Mod:phys3#Appendix_1). This is a result of the gauche conformer increasing the entropy of the system, which is favourable.&lt;br /&gt;
&lt;br /&gt;
The initial anti and gauche conformations are shown right (click to enlarge; links to 3D JMols).&lt;br /&gt;
&lt;br /&gt;
*Note: the numbering of gauche conformations in the table below does not intend to correspond with the numbering on the reference table &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforsresults.jpg|center|800 x 300 px|thumb|Conformations of hexadiene.]]&lt;br /&gt;
&lt;br /&gt;
A further anti conformation has been modelled also, shown right. The Ci (symmetry) anti2 conformation of 1,5-hexadiene has been optimised at both the HF/3-21G and B3LYP/6-31G* level, the energies are tabulated below. There is essentially no difference between the geometry of the two structures, but a large difference in energy. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforsresults2.jpg|center|300 x 150 px|thumb|Anti conformations of hexadiene: differing basis sets.]]&lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the structures to be minimal energy (vibrational frequecies are the second derivative of energy, being real and positive thus corresponds to a minima point). For the higher level calculation, the &#039;low frequencies&#039; are:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---   -9.4888   -0.0006   -0.0006    0.0002    3.7552   13.0176&lt;br /&gt;
 Low frequencies ---   74.2853   80.9980  121.4178&lt;br /&gt;
&lt;br /&gt;
The infrared spectrum is shown right. The vibrational analysis also computes real properties that may be compared:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=           -234.469204&lt;br /&gt;
 Sum of electronic and thermal Energies=              -234.461857&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=            -234.460913&lt;br /&gt;
 Sum of electronic and thermal Free Energies=         -234.500777&lt;br /&gt;
&lt;br /&gt;
The first of these is the potential energy at 0 K including the zero-point vibrational energy (E = Eelec + ZPE), the second is the energy at 298.15 K and 1 atm of pressure which includes contributions from the translational, rotational, and vibrational energy modes at this temperature (E = E + Evib + Erot + Etrans), the third contains an additional correction for RT (H = E + RT) which is particularly important when looking at dissociation reactions, and the last includes the entropic contribution to the free energy (G = H - TS).&lt;br /&gt;
&lt;br /&gt;
===Optimising the chair and boat transition structures===&lt;br /&gt;
[[Image:jr407m3p2conforms.jpg|right|200 x 200 px|thumb|The conformations of cyclohexane (http://wps.prenhall.com/wps/media/objects/724/741576/).]]&lt;br /&gt;
[[Image:jr407m3p2conformchair.jpg|right|200 x 200 px|thumb|Modelling the chair transition state.]]&lt;br /&gt;
The chair and boat conformations of cyclohexane are illustrated right (also showing their relative energies), as transition states the atoms are in these arrangements with bond being made and broken.  &lt;br /&gt;
&lt;br /&gt;
====Optimisation to a TS (Berny; chair)====&lt;br /&gt;
Initially the delocalised allyl fragment (CH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;CHCH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) was optimised (HF/3-21G) and configured in the assumed chair transition state (terminal C&#039;s approx. 2.2a.u. apart): this is shown right. A vibrational analysis was performed, revealing an imaginary vibration at 818cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; corresponding to the Cope rearrangement - this is shown below; the optimised transition state structure is shown right, with a distance of 2.02a.u. between the terminal carbons of each fragment.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p2chairir.jpg|center|400 x 200 px|thumb|Vibrational analysis of chair transition state.]]&lt;br /&gt;
&lt;br /&gt;
====Frozen coordinate method (chair)====&lt;br /&gt;
The transition state optimisation was repeated with frozen coordinates (the bond distance between the terminal carbons fixed), this was then repeated with the frozen coordinate bond as a derivative (no force constants calculated). The optimised lengths of the bond forming/breaking is retained at 2.02a.u. This corresponds to the chair transition state, with the same appearance as that of the TS (Berny) method, shown right.&lt;br /&gt;
&lt;br /&gt;
====QST2 method (boat)====&lt;br /&gt;
[[Image:jr407m3p2nunbersnumbers.jpg|right|200 x 200 px|thumb|Carbon numbering.]]&lt;br /&gt;
The boat transition state is optimised by the QST2 method: specifying the reactant and product structures, with the calculation interpolating between the two; crucial to this is a numbering of the carbons in the reactant and product that match. This method is not possible with the anti conformer of the reactant as rotation about the central bond is not possible and a transition state corresponds not to the Cope rearrangement. However, adjusting the reactant geometries allows for a boat transition state. This is illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p2confomersqst2.jpg|center|400 x 200 px|thumb|QST2 transition state determination.]]&lt;br /&gt;
&lt;br /&gt;
The bottom carbons of the fragments are separated &#039;through space&#039; by 2.14a.u., CC distances in the fragments 1.38a.u.; the further apart carbons at the top of each fragment are separated by 2.78a.u. through space.&lt;br /&gt;
&lt;br /&gt;
===Intermediate reaction coordinate analysis===&lt;br /&gt;
[[Image:jr407m3p4nomingra.jpg|right|200 x 200 px|thumb|Inititally a minima is not achieved.]]&lt;br /&gt;
&lt;br /&gt;
The optimised chair and boat transition structures connect conformers of 1,5-hexadiene, though by visual inspection it is nearly impossible to tell which ones. This is determined instead by following the minimum enery path from the transition state down to the local minimum (reactants) on a potential energy surface (intrinsic reaction coordinate [IRC] method in Gaussian). &lt;br /&gt;
&lt;br /&gt;
Force constants have been determined once at the beggining of the calculation, running the reaction coordinate in just the forward direction (since this is symmetrical), with 50 points. Initially a minimum is not reached (the gradient does not fall to zero - see graph, right), leaving three options:&lt;br /&gt;
*take the last point on the IRC and run a normal minimization (may lead to a local minima)&lt;br /&gt;
*restart the IRC and specify a larger number of points until it reaches a minimum (if not enough points, again a local minima)&lt;br /&gt;
*redo the IRC specifying to compute the force constants at every step (expensive and infeasible for large systems)&lt;br /&gt;
&lt;br /&gt;
The third option has been implemented, revealing the chair to result from conformer gauche 2 (see reference table: https://www.ch.ic.ac.uk/wiki/index.php/Mod:phys3) and the boat from a rather higher energy totally eclipsed conformer, resembling that used for the modified QST2 calculations above (a minimum was not achieved here, even using 100 iteration points). &lt;br /&gt;
&lt;br /&gt;
The reaction coordinate paths for the chair and boat transition states are illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p3chairirc.jpg|center|1000 x 500 px|thumb|IRC method: chair and boat transition states.]]&lt;br /&gt;
&lt;br /&gt;
===Higher level optimisation to determine activation energies===&lt;br /&gt;
[[Image:jr407m3p5631goptchair.jpg|thumb|right|6-31G* TS&#039;s.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Optchair631gJMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Chair TS (6-31G*) - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:Jr407m3p5631goptboat.jpg|thumb|right|Gauche Hexadiene - click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Optboat631gjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Boat TS (6-31G*) - 3D JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
The chair and boat transition structures have been reoptimised at the higher B3LYP/6-31G* level of theory, these are shown right with links to 3D JMols (note these return the structure to a localised bonding representation). The energies of the transition structures are both levels of theory are tabulated below and activation energies calculated, at the higher level of theory these are in fair aggreement with the experimental values (0K) when accounting for error, being no more than 1 kcal/mol out. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p5tableacen.jpg|center|800 x 300 px|thumb|Activation energies; note: 1 a.u. = 627.509 kcal/mol.]]&lt;br /&gt;
&lt;br /&gt;
A geometry analysis has also been performed, investigating the through space separation of the fragments in the transition state, and C-C bond lengths within the fragments at the different levels of theory. These are tabulated (and illustrated) below.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p5tabgeocompts.jpg|center|800 x 300 px|thumb|Geometric comparison of transition states.]]&lt;br /&gt;
&lt;br /&gt;
In summary the geometry changes minimally at the higher level of theory, while the molecules are greatly stabilised and found to have much lower energies (more accurate also, being a better agreement with experimental data for activation energy).&lt;br /&gt;
&lt;br /&gt;
==Mini-Project==&lt;br /&gt;
A mini-project in transition state computational chemistry has been conducted based on the Diels-Alder cycloaddition. &lt;br /&gt;
&lt;br /&gt;
The projects should be viewed here: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073PROJECT.&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details).&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan Engineering College - Transition State Theory: http://www.engin.umich.edu/]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;br /&gt;
* [Mini-project: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073PROJECT]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073&amp;diff=85551</id>
		<title>Rep:Namespace:jr4073</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073&amp;diff=85551"/>
		<updated>2009-12-18T11:14:40Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Conformational analysis of hexadiene */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstates.jpg|thumb|left|200px|Transition State Theory (Michigan Engineering College)]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Computational Chemistry - Introduction and application...&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Computational chemistry allows us to model transition states and potential energy surfaces to predict reactivity, which has many applications, illustrated here with the Cope rearrangement and Diels Alder cycloaddition reactions.  &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;Computational Chemistry - Module 3: Physical&#039;&#039;&#039;=&lt;br /&gt;
The first section of this investigation illustrates the virtues of computational methods in determining transition states, using the Cope Rearrangement as an example. The mini-project that follows then applies these methods to deduce new conclusions. &lt;br /&gt;
&lt;br /&gt;
==Cope Rearrangement==&lt;br /&gt;
[[Image:jr407m3p1cope.jpg|thumb|right|The Cope rearrangement.]]&lt;br /&gt;
&lt;br /&gt;
Computational methods are used to investigate transition states (potential energy minima) for the Cope rearrangement of 1,5-hexadiene to determine the preferred mechanism (step-wise, dissociative or concerted). This is begun with a conformational analysis of the reactants before considering transition state geometry (chair or boat). &lt;br /&gt;
&lt;br /&gt;
===Conformational analysis of hexadiene===&lt;br /&gt;
[[Image:jr407m3p1apph.jpg|thumb|right|Anti Hexadiene- click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Jr407Hexadienejmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Anti Hexadiene3D - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3p1gaucheh.jpg|thumb|right|Gauche Hexadiene - click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Hexadienechemgauchejmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Gauche Hexadiene - 3D JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3p1anti2dft.jpg|thumb|right|Anti2 conformation (hexadiene).]]&lt;br /&gt;
[[Image:jr407m3p1anti2ir.jpg|thumb|right|IR spectra (anti2 hexadiene).]]&lt;br /&gt;
&lt;br /&gt;
Molecules may exist in various conformations, of differing energies. For substituted carbons these may be termed depending upon the arrangement of substituents relative to each other, this is illustrated below by Newman projection.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforexam.jpg|center|800 x 300 px|thumb|Conformational analysis: butane in example.]]&lt;br /&gt;
&lt;br /&gt;
1,5-hexadiene has been geometry optimised in Gaussian (method: Hartree-Fock [HF]; basis set: 3-21G) for both the anti and gauche conformation (of the central four C atoms); the %mem term has been set at 250MB and 500MB for both calculations, showing no difference in the results. The energy and symmetry (point group) of the optimised structures are tabulated below. One would expect the gauche conformation to be at a higher energy, and this is the initial result. However, a number of possible gauche structures can be imagined, and these have also been optimised, identifying a gauche conformation at lower energy than the anti, which match the reference structures (https://www.ch.ic.ac.uk/wiki/index.php/Mod:phys3#Appendix_1). This is a result of the gauche conformer increasing the entropy of the system, which is favourable.&lt;br /&gt;
&lt;br /&gt;
The initial anti and gauche conformations are shown right (click to enlarge; links to 3D JMols).&lt;br /&gt;
&lt;br /&gt;
*Note: the numbering of gauche conformations in the table below does not intend to correspond with the numbering on the reference table &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforsresults.jpg|center|800 x 300 px|thumb|Conformations of hexadiene.]]&lt;br /&gt;
&lt;br /&gt;
The Ci (symmetry) anti2 conformation of 1,5-hexadiene has been optimised at both the HF/3-21G and B3LYP/6-31G* level, the energies are tabulated below. There is essentially no difference between the geometry of the two structures, but a large difference in energy. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforsresults2.jpg|center|300 x 150 px|thumb|Anti conformations of hexadiene: differing basis sets.]]&lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the structures to be minimal energy (vibrational frequecies are the second derivative of energy, being real and positive thus corresponds to a minima point). For the higher level calculation, the &#039;low frequencies&#039; are:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---   -9.4888   -0.0006   -0.0006    0.0002    3.7552   13.0176&lt;br /&gt;
 Low frequencies ---   74.2853   80.9980  121.4178&lt;br /&gt;
&lt;br /&gt;
The infrared spectrum is shown right. The vibrational analysis also computes real properties that may be compared:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=           -234.469204&lt;br /&gt;
 Sum of electronic and thermal Energies=              -234.461857&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=            -234.460913&lt;br /&gt;
 Sum of electronic and thermal Free Energies=         -234.500777&lt;br /&gt;
&lt;br /&gt;
The first of these is the potential energy at 0 K including the zero-point vibrational energy (E = Eelec + ZPE), the second is the energy at 298.15 K and 1 atm of pressure which includes contributions from the translational, rotational, and vibrational energy modes at this temperature (E = E + Evib + Erot + Etrans), the third contains an additional correction for RT (H = E + RT) which is particularly important when looking at dissociation reactions, and the last includes the entropic contribution to the free energy (G = H - TS).&lt;br /&gt;
&lt;br /&gt;
===Optimising the chair and boat transition structures===&lt;br /&gt;
[[Image:jr407m3p2conforms.jpg|right|200 x 200 px|thumb|The conformations of cyclohexane (http://wps.prenhall.com/wps/media/objects/724/741576/).]]&lt;br /&gt;
[[Image:jr407m3p2conformchair.jpg|right|200 x 200 px|thumb|Modelling the chair transition state.]]&lt;br /&gt;
The chair and boat conformations of cyclohexane are illustrated right (also showing their relative energies), as transition states the atoms are in these arrangements with bond being made and broken.  &lt;br /&gt;
&lt;br /&gt;
====Optimisation to a TS (Berny; chair)====&lt;br /&gt;
Initially the delocalised allyl fragment (CH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;CHCH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) was optimised (HF/3-21G) and configured in the assumed chair transition state (terminal C&#039;s approx. 2.2a.u. apart): this is shown right. A vibrational analysis was performed, revealing an imaginary vibration at 818cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; corresponding to the Cope rearrangement - this is shown below; the optimised transition state structure is shown right, with a distance of 2.02a.u. between the terminal carbons of each fragment.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p2chairir.jpg|center|400 x 200 px|thumb|Vibrational analysis of chair transition state.]]&lt;br /&gt;
&lt;br /&gt;
====Frozen coordinate method (chair)====&lt;br /&gt;
The transition state optimisation was repeated with frozen coordinates (the bond distance between the terminal carbons fixed), this was then repeated with the frozen coordinate bond as a derivative (no force constants calculated). The optimised lengths of the bond forming/breaking is retained at 2.02a.u. This corresponds to the chair transition state, with the same appearance as that of the TS (Berny) method, shown right.&lt;br /&gt;
&lt;br /&gt;
====QST2 method (boat)====&lt;br /&gt;
[[Image:jr407m3p2nunbersnumbers.jpg|right|200 x 200 px|thumb|Carbon numbering.]]&lt;br /&gt;
The boat transition state is optimised by the QST2 method: specifying the reactant and product structures, with the calculation interpolating between the two; crucial to this is a numbering of the carbons in the reactant and product that match. This method is not possible with the anti conformer of the reactant as rotation about the central bond is not possible and a transition state corresponds not to the Cope rearrangement. However, adjusting the reactant geometries allows for a boat transition state. This is illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p2confomersqst2.jpg|center|400 x 200 px|thumb|QST2 transition state determination.]]&lt;br /&gt;
&lt;br /&gt;
The bottom carbons of the fragments are separated &#039;through space&#039; by 2.14a.u., CC distances in the fragments 1.38a.u.; the further apart carbons at the top of each fragment are separated by 2.78a.u. through space.&lt;br /&gt;
&lt;br /&gt;
===Intermediate reaction coordinate analysis===&lt;br /&gt;
[[Image:jr407m3p4nomingra.jpg|right|200 x 200 px|thumb|Inititally a minima is not achieved.]]&lt;br /&gt;
&lt;br /&gt;
The optimised chair and boat transition structures connect conformers of 1,5-hexadiene, though by visual inspection it is nearly impossible to tell which ones. This is determined instead by following the minimum enery path from the transition state down to the local minimum (reactants) on a potential energy surface (intrinsic reaction coordinate [IRC] method in Gaussian). &lt;br /&gt;
&lt;br /&gt;
Force constants have been determined once at the beggining of the calculation, running the reaction coordinate in just the forward direction (since this is symmetrical), with 50 points. Initially a minimum is not reached (the gradient does not fall to zero - see graph, right), leaving three options:&lt;br /&gt;
*take the last point on the IRC and run a normal minimization (may lead to a local minima)&lt;br /&gt;
*restart the IRC and specify a larger number of points until it reaches a minimum (if not enough points, again a local minima)&lt;br /&gt;
*redo the IRC specifying to compute the force constants at every step (expensive and infeasible for large systems)&lt;br /&gt;
&lt;br /&gt;
The third option has been implemented, revealing the chair to result from conformer gauche 2 (see reference table: https://www.ch.ic.ac.uk/wiki/index.php/Mod:phys3) and the boat from a rather higher energy totally eclipsed conformer, resembling that used for the modified QST2 calculations above (a minimum was not achieved here, even using 100 iteration points). &lt;br /&gt;
&lt;br /&gt;
The reaction coordinate paths for the chair and boat transition states are illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p3chairirc.jpg|center|1000 x 500 px|thumb|IRC method: chair and boat transition states.]]&lt;br /&gt;
&lt;br /&gt;
===Higher level optimisation to determine activation energies===&lt;br /&gt;
[[Image:jr407m3p5631goptchair.jpg|thumb|right|6-31G* TS&#039;s.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Optchair631gJMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Chair TS (6-31G*) - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:Jr407m3p5631goptboat.jpg|thumb|right|Gauche Hexadiene - click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Optboat631gjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Boat TS (6-31G*) - 3D JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
The chair and boat transition structures have been reoptimised at the higher B3LYP/6-31G* level of theory, these are shown right with links to 3D JMols (note these return the structure to a localised bonding representation). The energies of the transition structures are both levels of theory are tabulated below and activation energies calculated, at the higher level of theory these are in fair aggreement with the experimental values (0K) when accounting for error, being no more than 1 kcal/mol out. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p5tableacen.jpg|center|800 x 300 px|thumb|Activation energies; note: 1 a.u. = 627.509 kcal/mol.]]&lt;br /&gt;
&lt;br /&gt;
A geometry analysis has also been performed, investigating the through space separation of the fragments in the transition state, and C-C bond lengths within the fragments at the different levels of theory. These are tabulated (and illustrated) below.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p5tabgeocompts.jpg|center|800 x 300 px|thumb|Geometric comparison of transition states.]]&lt;br /&gt;
&lt;br /&gt;
In summary the geometry changes minimally at the higher level of theory, while the molecules are greatly stabilised and found to have much lower energies (more accurate also, being a better agreement with experimental data for activation energy).&lt;br /&gt;
&lt;br /&gt;
==Mini-Project==&lt;br /&gt;
A mini-project in transition state computational chemistry has been conducted based on the Diels-Alder cycloaddition. &lt;br /&gt;
&lt;br /&gt;
The projects should be viewed here: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073PROJECT.&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details).&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan Engineering College - Transition State Theory: http://www.engin.umich.edu/]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;br /&gt;
* [Mini-project: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073PROJECT]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073&amp;diff=85550</id>
		<title>Rep:Namespace:jr4073</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073&amp;diff=85550"/>
		<updated>2009-12-18T11:13:32Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Conformational analysis of hexadiene */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstates.jpg|thumb|left|200px|Transition State Theory (Michigan Engineering College)]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Computational Chemistry - Introduction and application...&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Computational chemistry allows us to model transition states and potential energy surfaces to predict reactivity, which has many applications, illustrated here with the Cope rearrangement and Diels Alder cycloaddition reactions.  &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;Computational Chemistry - Module 3: Physical&#039;&#039;&#039;=&lt;br /&gt;
The first section of this investigation illustrates the virtues of computational methods in determining transition states, using the Cope Rearrangement as an example. The mini-project that follows then applies these methods to deduce new conclusions. &lt;br /&gt;
&lt;br /&gt;
==Cope Rearrangement==&lt;br /&gt;
[[Image:jr407m3p1cope.jpg|thumb|right|The Cope rearrangement.]]&lt;br /&gt;
&lt;br /&gt;
Computational methods are used to investigate transition states (potential energy minima) for the Cope rearrangement of 1,5-hexadiene to determine the preferred mechanism (step-wise, dissociative or concerted). This is begun with a conformational analysis of the reactants before considering transition state geometry (chair or boat). &lt;br /&gt;
&lt;br /&gt;
===Conformational analysis of hexadiene===&lt;br /&gt;
[[Image:jr407m3p1apph.jpg|thumb|right|Anti Hexadiene- click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Jr407Hexadienejmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Anti Hexadiene3D - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3p1gaucheh.jpg|thumb|right|Gauche Hexadiene - click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Hexadienechemgauchejmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Gauche Hexadiene - 3D JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3p1anti2dft.jpg|thumb|right|Anti2 conformation (hexadiene).]]&lt;br /&gt;
[[Image:jr407m3p1anti2ir.jpg|thumb|right|IR spectra (anti2 hexadiene).]]&lt;br /&gt;
&lt;br /&gt;
Molecules may exist in various conformations, of differing energies. For substituted carbons these may be termed depending upon the arrangement of substituents relative to each other, this is illustrated below by Newman projection.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforexam.jpg|center|800 x 300 px|thumb|Conformational analysis: butane in example.]]&lt;br /&gt;
&lt;br /&gt;
1,5-hexadiene has been geometry optimised in Gaussian (method: Hartree-Fock [HF]; basis set: 3-21G) for both the anti and gauche conformation (of the central four C atoms); the %mem term has been set at 250MB and 500MB for both calculations, showing no difference in the results. The energy and symmetry (point group) of the optimised structures are tabulated below. One would expect the gauche conformation to be at a higher energy, and this is the initial result. However, a number of possible gauche structures can be imagined, and these have also been optimised, identifying a gauche conformation at lower energy than the anti, which match the reference structures (https://www.ch.ic.ac.uk/wiki/index.php/Mod:phys3#Appendix_1). &lt;br /&gt;
&lt;br /&gt;
The initial anti and gauche conformations are shown right (click to enlarge; links to 3D JMols).&lt;br /&gt;
&lt;br /&gt;
*Note: the numbering of gauche conformations in the table below does not intend to correspond with the numbering on the reference table &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforsresults.jpg|center|800 x 300 px|thumb|Conformations of hexadiene.]]&lt;br /&gt;
&lt;br /&gt;
The Ci (symmetry) anti2 conformation of 1,5-hexadiene has been optimised at both the HF/3-21G and B3LYP/6-31G* level, the energies are tabulated below. There is essentially no difference between the geometry of the two structures, but a large difference in energy. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforsresults2.jpg|center|300 x 150 px|thumb|Anti conformations of hexadiene: differing basis sets.]]&lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the structures to be minimal energy (vibrational frequecies are the second derivative of energy, being real and positive thus corresponds to a minima point). For the higher level calculation, the &#039;low frequencies&#039; are:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---   -9.4888   -0.0006   -0.0006    0.0002    3.7552   13.0176&lt;br /&gt;
 Low frequencies ---   74.2853   80.9980  121.4178&lt;br /&gt;
&lt;br /&gt;
The infrared spectrum is shown right. The vibrational analysis also computes real properties that may be compared:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=           -234.469204&lt;br /&gt;
 Sum of electronic and thermal Energies=              -234.461857&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=            -234.460913&lt;br /&gt;
 Sum of electronic and thermal Free Energies=         -234.500777&lt;br /&gt;
&lt;br /&gt;
The first of these is the potential energy at 0 K including the zero-point vibrational energy (E = Eelec + ZPE), the second is the energy at 298.15 K and 1 atm of pressure which includes contributions from the translational, rotational, and vibrational energy modes at this temperature (E = E + Evib + Erot + Etrans), the third contains an additional correction for RT (H = E + RT) which is particularly important when looking at dissociation reactions, and the last includes the entropic contribution to the free energy (G = H - TS).&lt;br /&gt;
&lt;br /&gt;
===Optimising the chair and boat transition structures===&lt;br /&gt;
[[Image:jr407m3p2conforms.jpg|right|200 x 200 px|thumb|The conformations of cyclohexane (http://wps.prenhall.com/wps/media/objects/724/741576/).]]&lt;br /&gt;
[[Image:jr407m3p2conformchair.jpg|right|200 x 200 px|thumb|Modelling the chair transition state.]]&lt;br /&gt;
The chair and boat conformations of cyclohexane are illustrated right (also showing their relative energies), as transition states the atoms are in these arrangements with bond being made and broken.  &lt;br /&gt;
&lt;br /&gt;
====Optimisation to a TS (Berny; chair)====&lt;br /&gt;
Initially the delocalised allyl fragment (CH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;CHCH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) was optimised (HF/3-21G) and configured in the assumed chair transition state (terminal C&#039;s approx. 2.2a.u. apart): this is shown right. A vibrational analysis was performed, revealing an imaginary vibration at 818cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; corresponding to the Cope rearrangement - this is shown below; the optimised transition state structure is shown right, with a distance of 2.02a.u. between the terminal carbons of each fragment.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p2chairir.jpg|center|400 x 200 px|thumb|Vibrational analysis of chair transition state.]]&lt;br /&gt;
&lt;br /&gt;
====Frozen coordinate method (chair)====&lt;br /&gt;
The transition state optimisation was repeated with frozen coordinates (the bond distance between the terminal carbons fixed), this was then repeated with the frozen coordinate bond as a derivative (no force constants calculated). The optimised lengths of the bond forming/breaking is retained at 2.02a.u. This corresponds to the chair transition state, with the same appearance as that of the TS (Berny) method, shown right.&lt;br /&gt;
&lt;br /&gt;
====QST2 method (boat)====&lt;br /&gt;
[[Image:jr407m3p2nunbersnumbers.jpg|right|200 x 200 px|thumb|Carbon numbering.]]&lt;br /&gt;
The boat transition state is optimised by the QST2 method: specifying the reactant and product structures, with the calculation interpolating between the two; crucial to this is a numbering of the carbons in the reactant and product that match. This method is not possible with the anti conformer of the reactant as rotation about the central bond is not possible and a transition state corresponds not to the Cope rearrangement. However, adjusting the reactant geometries allows for a boat transition state. This is illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p2confomersqst2.jpg|center|400 x 200 px|thumb|QST2 transition state determination.]]&lt;br /&gt;
&lt;br /&gt;
The bottom carbons of the fragments are separated &#039;through space&#039; by 2.14a.u., CC distances in the fragments 1.38a.u.; the further apart carbons at the top of each fragment are separated by 2.78a.u. through space.&lt;br /&gt;
&lt;br /&gt;
===Intermediate reaction coordinate analysis===&lt;br /&gt;
[[Image:jr407m3p4nomingra.jpg|right|200 x 200 px|thumb|Inititally a minima is not achieved.]]&lt;br /&gt;
&lt;br /&gt;
The optimised chair and boat transition structures connect conformers of 1,5-hexadiene, though by visual inspection it is nearly impossible to tell which ones. This is determined instead by following the minimum enery path from the transition state down to the local minimum (reactants) on a potential energy surface (intrinsic reaction coordinate [IRC] method in Gaussian). &lt;br /&gt;
&lt;br /&gt;
Force constants have been determined once at the beggining of the calculation, running the reaction coordinate in just the forward direction (since this is symmetrical), with 50 points. Initially a minimum is not reached (the gradient does not fall to zero - see graph, right), leaving three options:&lt;br /&gt;
*take the last point on the IRC and run a normal minimization (may lead to a local minima)&lt;br /&gt;
*restart the IRC and specify a larger number of points until it reaches a minimum (if not enough points, again a local minima)&lt;br /&gt;
*redo the IRC specifying to compute the force constants at every step (expensive and infeasible for large systems)&lt;br /&gt;
&lt;br /&gt;
The third option has been implemented, revealing the chair to result from conformer gauche 2 (see reference table: https://www.ch.ic.ac.uk/wiki/index.php/Mod:phys3) and the boat from a rather higher energy totally eclipsed conformer, resembling that used for the modified QST2 calculations above (a minimum was not achieved here, even using 100 iteration points). &lt;br /&gt;
&lt;br /&gt;
The reaction coordinate paths for the chair and boat transition states are illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p3chairirc.jpg|center|1000 x 500 px|thumb|IRC method: chair and boat transition states.]]&lt;br /&gt;
&lt;br /&gt;
===Higher level optimisation to determine activation energies===&lt;br /&gt;
[[Image:jr407m3p5631goptchair.jpg|thumb|right|6-31G* TS&#039;s.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Optchair631gJMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Chair TS (6-31G*) - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:Jr407m3p5631goptboat.jpg|thumb|right|Gauche Hexadiene - click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Optboat631gjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Boat TS (6-31G*) - 3D JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
The chair and boat transition structures have been reoptimised at the higher B3LYP/6-31G* level of theory, these are shown right with links to 3D JMols (note these return the structure to a localised bonding representation). The energies of the transition structures are both levels of theory are tabulated below and activation energies calculated, at the higher level of theory these are in fair aggreement with the experimental values (0K) when accounting for error, being no more than 1 kcal/mol out. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p5tableacen.jpg|center|800 x 300 px|thumb|Activation energies; note: 1 a.u. = 627.509 kcal/mol.]]&lt;br /&gt;
&lt;br /&gt;
A geometry analysis has also been performed, investigating the through space separation of the fragments in the transition state, and C-C bond lengths within the fragments at the different levels of theory. These are tabulated (and illustrated) below.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p5tabgeocompts.jpg|center|800 x 300 px|thumb|Geometric comparison of transition states.]]&lt;br /&gt;
&lt;br /&gt;
In summary the geometry changes minimally at the higher level of theory, while the molecules are greatly stabilised and found to have much lower energies (more accurate also, being a better agreement with experimental data for activation energy).&lt;br /&gt;
&lt;br /&gt;
==Mini-Project==&lt;br /&gt;
A mini-project in transition state computational chemistry has been conducted based on the Diels-Alder cycloaddition. &lt;br /&gt;
&lt;br /&gt;
The projects should be viewed here: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073PROJECT.&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details).&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan Engineering College - Transition State Theory: http://www.engin.umich.edu/]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;br /&gt;
* [Mini-project: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073PROJECT]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85546</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85546"/>
		<updated>2009-12-18T11:09:58Z</updated>

		<summary type="html">&lt;p&gt;Jr407: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result, and semi-empirical (AM1) calculations to show MOs.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
[[Image:jr407methylenemos.jpg|thumb|right|Ethylene MOs]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right). The optimised molecule is fully planar with a dihedral angle of 0deg (C-C-C-C).&lt;br /&gt;
&lt;br /&gt;
The MOs of ethylene have also been computed in the same manner (shown right), the HOMO being symmetric and the LUMO anti-symmetric this time though, with no nodal planes in the HOMO and one in the LUMO.&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; bonded carbon has a C-C bondlength of 1.54Å, and sp&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
Notably the LUMO of the transition state is formed by the combination of the ethylene HOMO and cis-butadiene LUMO (both symmetric, s); the ethylene HOMO and LUMO are of course the pi and pi* bonding and anti-bonding MOs. The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|400 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details).&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Main Page: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073]&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073&amp;diff=85543</id>
		<title>Rep:Namespace:jr4073</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073&amp;diff=85543"/>
		<updated>2009-12-18T11:08:35Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Error analysis... */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstates.jpg|thumb|left|200px|Transition State Theory (Michigan Engineering College)]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Computational Chemistry - Introduction and application...&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Computational chemistry allows us to model transition states and potential energy surfaces to predict reactivity, which has many applications, illustrated here with the Cope rearrangement and Diels Alder cycloaddition reactions.  &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;Computational Chemistry - Module 3: Physical&#039;&#039;&#039;=&lt;br /&gt;
The first section of this investigation illustrates the virtues of computational methods in determining transition states, using the Cope Rearrangement as an example. The mini-project that follows then applies these methods to deduce new conclusions. &lt;br /&gt;
&lt;br /&gt;
==Cope Rearrangement==&lt;br /&gt;
[[Image:jr407m3p1cope.jpg|thumb|right|The Cope rearrangement.]]&lt;br /&gt;
&lt;br /&gt;
Computational methods are used to investigate transition states (potential energy minima) for the Cope rearrangement of 1,5-hexadiene to determine the preferred mechanism (step-wise, dissociative or concerted). This is begun with a conformational analysis of the reactants before considering transition state geometry (chair or boat). &lt;br /&gt;
&lt;br /&gt;
===Conformational analysis of hexadiene===&lt;br /&gt;
[[Image:jr407m3p1apph.jpg|thumb|right|Anti Hexadiene- click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Jr407Hexadienejmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Anti Hexadiene3D - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3p1gaucheh.jpg|thumb|right|Gauche Hexadiene - click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Hexadienechemgauchejmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Gauche Hexadiene - 3D JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3p1anti2dft.jpg|thumb|right|Anti2 conformation (hexadiene).]]&lt;br /&gt;
[[Image:jr407m3p1anti2ir.jpg|thumb|right|IR spectra (anti2 hexadiene).]]&lt;br /&gt;
&lt;br /&gt;
Molecules may exist in various conformations, of differing energies. For substituted carbons these may be termed depending upon the arrangement of substituents relative to each other, this is illustrated below by Newman projection.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforexam.jpg|center|800 x 300 px|thumb|Conformational analysis: butane in example.]]&lt;br /&gt;
&lt;br /&gt;
1,5-hexadiene has been geometry optimised in Gaussian (method: Hartree-Fock [HF]; basis set: 3-21G) for both the anti and gauche conformation (of the central four C atoms); the %mem term has been set at 250MB and 500MB for both calculations, showing no difference in the results. The energy and symmetry (point group) of the optimised structures are tabulated below. One would expect the gauche conformation to be at a higher energy, and this is the initial result. However, a number of possible gauche structures can be imagined, and these have also been optimised, identifying a gauche conformation at lower energy than the anti, which match the reference structures (https://www.ch.ic.ac.uk/wiki/index.php/Mod:phys3#Appendix_1). &lt;br /&gt;
&lt;br /&gt;
The initial anti and gauche conformations are shown right (click to enlarge; links to 3D JMols).&lt;br /&gt;
&lt;br /&gt;
*Note: the numbering of gauche conformations in the table below does not intend to correspond with the numbering on the reference table &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforsresults.jpg|center|800 x 300 px|thumb|Conformations of hexadiene.]]&lt;br /&gt;
&lt;br /&gt;
The Ci (symmetry) anti2 conformation of 1,5-hexadiene has been optimised at both the HF/3-21G and B3LYP/6-31G* level, the energies are tabulated below. There is essentially no difference between the geometry of the two structures. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p1hconforsresults2.jpg|center|300 x 150 px|thumb|Anti conformations of hexadiene: differing basis sets.]]&lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the structures to be minimal energy (vibrational frequecies are the second derivative of energy, being real and positive thus corresponds to a minima point). For the higher level calculation, the &#039;low frequencies&#039; are:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---   -9.4888   -0.0006   -0.0006    0.0002    3.7552   13.0176&lt;br /&gt;
 Low frequencies ---   74.2853   80.9980  121.4178&lt;br /&gt;
&lt;br /&gt;
The infrared spectrum is shown right. The vibrational analysis also computes real properties that may be compared:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=           -234.469204&lt;br /&gt;
 Sum of electronic and thermal Energies=              -234.461857&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=            -234.460913&lt;br /&gt;
 Sum of electronic and thermal Free Energies=         -234.500777&lt;br /&gt;
&lt;br /&gt;
The first of these is the potential energy at 0 K including the zero-point vibrational energy (E = Eelec + ZPE), the second is the energy at 298.15 K and 1 atm of pressure which includes contributions from the translational, rotational, and vibrational energy modes at this temperature (E = E + Evib + Erot + Etrans), the third contains an additional correction for RT (H = E + RT) which is particularly important when looking at dissociation reactions, and the last includes the entropic contribution to the free energy (G = H - TS).&lt;br /&gt;
&lt;br /&gt;
===Optimising the chair and boat transition structures===&lt;br /&gt;
[[Image:jr407m3p2conforms.jpg|right|200 x 200 px|thumb|The conformations of cyclohexane (http://wps.prenhall.com/wps/media/objects/724/741576/).]]&lt;br /&gt;
[[Image:jr407m3p2conformchair.jpg|right|200 x 200 px|thumb|Modelling the chair transition state.]]&lt;br /&gt;
The chair and boat conformations of cyclohexane are illustrated right (also showing their relative energies), as transition states the atoms are in these arrangements with bond being made and broken.  &lt;br /&gt;
&lt;br /&gt;
====Optimisation to a TS (Berny; chair)====&lt;br /&gt;
Initially the delocalised allyl fragment (CH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;CHCH&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) was optimised (HF/3-21G) and configured in the assumed chair transition state (terminal C&#039;s approx. 2.2a.u. apart): this is shown right. A vibrational analysis was performed, revealing an imaginary vibration at 818cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; corresponding to the Cope rearrangement - this is shown below; the optimised transition state structure is shown right, with a distance of 2.02a.u. between the terminal carbons of each fragment.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p2chairir.jpg|center|400 x 200 px|thumb|Vibrational analysis of chair transition state.]]&lt;br /&gt;
&lt;br /&gt;
====Frozen coordinate method (chair)====&lt;br /&gt;
The transition state optimisation was repeated with frozen coordinates (the bond distance between the terminal carbons fixed), this was then repeated with the frozen coordinate bond as a derivative (no force constants calculated). The optimised lengths of the bond forming/breaking is retained at 2.02a.u. This corresponds to the chair transition state, with the same appearance as that of the TS (Berny) method, shown right.&lt;br /&gt;
&lt;br /&gt;
====QST2 method (boat)====&lt;br /&gt;
[[Image:jr407m3p2nunbersnumbers.jpg|right|200 x 200 px|thumb|Carbon numbering.]]&lt;br /&gt;
The boat transition state is optimised by the QST2 method: specifying the reactant and product structures, with the calculation interpolating between the two; crucial to this is a numbering of the carbons in the reactant and product that match. This method is not possible with the anti conformer of the reactant as rotation about the central bond is not possible and a transition state corresponds not to the Cope rearrangement. However, adjusting the reactant geometries allows for a boat transition state. This is illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p2confomersqst2.jpg|center|400 x 200 px|thumb|QST2 transition state determination.]]&lt;br /&gt;
&lt;br /&gt;
The bottom carbons of the fragments are separated &#039;through space&#039; by 2.14a.u., CC distances in the fragments 1.38a.u.; the further apart carbons at the top of each fragment are separated by 2.78a.u. through space.&lt;br /&gt;
&lt;br /&gt;
===Intermediate reaction coordinate analysis===&lt;br /&gt;
[[Image:jr407m3p4nomingra.jpg|right|200 x 200 px|thumb|Inititally a minima is not achieved.]]&lt;br /&gt;
&lt;br /&gt;
The optimised chair and boat transition structures connect conformers of 1,5-hexadiene, though by visual inspection it is nearly impossible to tell which ones. This is determined instead by following the minimum enery path from the transition state down to the local minimum (reactants) on a potential energy surface (intrinsic reaction coordinate [IRC] method in Gaussian). &lt;br /&gt;
&lt;br /&gt;
Force constants have been determined once at the beggining of the calculation, running the reaction coordinate in just the forward direction (since this is symmetrical), with 50 points. Initially a minimum is not reached (the gradient does not fall to zero - see graph, right), leaving three options:&lt;br /&gt;
*take the last point on the IRC and run a normal minimization (may lead to a local minima)&lt;br /&gt;
*restart the IRC and specify a larger number of points until it reaches a minimum (if not enough points, again a local minima)&lt;br /&gt;
*redo the IRC specifying to compute the force constants at every step (expensive and infeasible for large systems)&lt;br /&gt;
&lt;br /&gt;
The third option has been implemented, revealing the chair to result from conformer gauche 2 (see reference table: https://www.ch.ic.ac.uk/wiki/index.php/Mod:phys3) and the boat from a rather higher energy totally eclipsed conformer, resembling that used for the modified QST2 calculations above (a minimum was not achieved here, even using 100 iteration points). &lt;br /&gt;
&lt;br /&gt;
The reaction coordinate paths for the chair and boat transition states are illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p3chairirc.jpg|center|1000 x 500 px|thumb|IRC method: chair and boat transition states.]]&lt;br /&gt;
&lt;br /&gt;
===Higher level optimisation to determine activation energies===&lt;br /&gt;
[[Image:jr407m3p5631goptchair.jpg|thumb|right|6-31G* TS&#039;s.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Optchair631gJMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Chair TS (6-31G*) - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:Jr407m3p5631goptboat.jpg|thumb|right|Gauche Hexadiene - click to enlarge.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Optboat631gjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Boat TS (6-31G*) - 3D JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
The chair and boat transition structures have been reoptimised at the higher B3LYP/6-31G* level of theory, these are shown right with links to 3D JMols (note these return the structure to a localised bonding representation). The energies of the transition structures are both levels of theory are tabulated below and activation energies calculated, at the higher level of theory these are in fair aggreement with the experimental values (0K) when accounting for error, being no more than 1 kcal/mol out. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p5tableacen.jpg|center|800 x 300 px|thumb|Activation energies; note: 1 a.u. = 627.509 kcal/mol.]]&lt;br /&gt;
&lt;br /&gt;
A geometry analysis has also been performed, investigating the through space separation of the fragments in the transition state, and C-C bond lengths within the fragments at the different levels of theory. These are tabulated (and illustrated) below.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3p5tabgeocompts.jpg|center|800 x 300 px|thumb|Geometric comparison of transition states.]]&lt;br /&gt;
&lt;br /&gt;
In summary the geometry changes minimally at the higher level of theory, while the molecules are greatly stabilised and found to have much lower energies (more accurate also, being a better agreement with experimental data for activation energy).&lt;br /&gt;
&lt;br /&gt;
==Mini-Project==&lt;br /&gt;
A mini-project in transition state computational chemistry has been conducted based on the Diels-Alder cycloaddition. &lt;br /&gt;
&lt;br /&gt;
The projects should be viewed here: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073PROJECT.&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details).&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan Engineering College - Transition State Theory: http://www.engin.umich.edu/]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;br /&gt;
* [Mini-project: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073PROJECT]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85542</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85542"/>
		<updated>2009-12-18T11:08:17Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* External links */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
[[Image:jr407methylenemos.jpg|thumb|right|Ethylene MOs]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right). The optimised molecule is fully planar with a dihedral angle of 0deg (C-C-C-C).&lt;br /&gt;
&lt;br /&gt;
The MOs of ethylene have also been computed in the same manner (shown right), the HOMO being symmetric and the LUMO anti-symmetric this time though, with no nodal planes in the HOMO and one in the LUMO.&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; bonded carbon has a C-C bondlength of 1.54Å, and sp&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
Notably the LUMO of the transition state is formed by the combination of the ethylene HOMO and cis-butadiene LUMO (both symmetric, s); the ethylene HOMO and LUMO are of course the pi and pi* bonding and anti-bonding MOs. The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|400 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details).&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Main Page: https://www.ch.ic.ac.uk/wiki/index.php/Namespace:jr4073]&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85540</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85540"/>
		<updated>2009-12-18T11:07:35Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Error analysis... */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
[[Image:jr407methylenemos.jpg|thumb|right|Ethylene MOs]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right). The optimised molecule is fully planar with a dihedral angle of 0deg (C-C-C-C).&lt;br /&gt;
&lt;br /&gt;
The MOs of ethylene have also been computed in the same manner (shown right), the HOMO being symmetric and the LUMO anti-symmetric this time though, with no nodal planes in the HOMO and one in the LUMO.&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; bonded carbon has a C-C bondlength of 1.54Å, and sp&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
Notably the LUMO of the transition state is formed by the combination of the ethylene HOMO and cis-butadiene LUMO (both symmetric, s); the ethylene HOMO and LUMO are of course the pi and pi* bonding and anti-bonding MOs. The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|400 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details).&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85539</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85539"/>
		<updated>2009-12-18T11:05:18Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* MO analysis of cis-butadiene */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
[[Image:jr407methylenemos.jpg|thumb|right|Ethylene MOs]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right). The optimised molecule is fully planar with a dihedral angle of 0deg (C-C-C-C).&lt;br /&gt;
&lt;br /&gt;
The MOs of ethylene have also been computed in the same manner (shown right), the HOMO being symmetric and the LUMO anti-symmetric this time though, with no nodal planes in the HOMO and one in the LUMO.&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; bonded carbon has a C-C bondlength of 1.54Å, and sp&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
Notably the LUMO of the transition state is formed by the combination of the ethylene HOMO and cis-butadiene LUMO (both symmetric, s); the ethylene HOMO and LUMO are of course the pi and pi* bonding and anti-bonding MOs. The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|400 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407methylenemos.jpg&amp;diff=85537</id>
		<title>File:Jr407methylenemos.jpg</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407methylenemos.jpg&amp;diff=85537"/>
		<updated>2009-12-18T11:03:35Z</updated>

		<summary type="html">&lt;p&gt;Jr407: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85536</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85536"/>
		<updated>2009-12-18T11:03:26Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
[[Image:jr407methylenemos.jpg|thumb|right|Ethylene MOs]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right). The optimised molecule is fully planar with a dihedral angle of 0deg (C-C-C-C).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; bonded carbon has a C-C bondlength of 1.54Å, and sp&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
Notably the LUMO of the transition state is formed by the combination of the ethylene HOMO and cis-butadiene LUMO (both symmetric, s); the ethylene HOMO and LUMO are of course the pi and pi* bonding and anti-bonding MOs. The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|400 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85532</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85532"/>
		<updated>2009-12-18T10:57:58Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* MO analysis of cis-butadiene */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right). The optimised molecule is fully planar with a dihedral angle of 0deg (C-C-C-C).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; bonded carbon has a C-C bondlength of 1.54Å, and sp&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
Notably the LUMO of the transition state is formed by the combination of the ethylene HOMO and cis-butadiene LUMO (both symmetric, s); the ethylene HOMO and LUMO are of course the pi and pi* bonding and anti-bonding MOs. The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|400 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85531</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85531"/>
		<updated>2009-12-18T10:56:08Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; bonded carbon has a C-C bondlength of 1.54Å, and sp&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
Notably the LUMO of the transition state is formed by the combination of the ethylene HOMO and cis-butadiene LUMO (both symmetric, s); the ethylene HOMO and LUMO are of course the pi and pi* bonding and anti-bonding MOs. The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|400 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85529</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85529"/>
		<updated>2009-12-18T10:53:41Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; bonded carbon has a C-C bondlength of 1.54Å, and sp&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|400 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85527</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85527"/>
		<updated>2009-12-18T10:53:15Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|400 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85524</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85524"/>
		<updated>2009-12-18T10:51:32Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|400 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85521</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85521"/>
		<updated>2009-12-18T10:50:18Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|400 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
(There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3pexervibs1.jpg&amp;diff=85519</id>
		<title>File:Jr407m3pexervibs1.jpg</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3pexervibs1.jpg&amp;diff=85519"/>
		<updated>2009-12-18T10:49:51Z</updated>

		<summary type="html">&lt;p&gt;Jr407: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85518</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85518"/>
		<updated>2009-12-18T10:49:41Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
Vibrational analysis confirms the optimised structures to be transition states (by the presence of a negative [imaginary] vibration indicating a local [not global] minima). Animating this vibration for both structures shows correspondence to the reaction path to the products: as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexervibs1.jpg|center|600 x 300 px|thumb|Transition state imaginary vibrations.]]&lt;br /&gt;
&lt;br /&gt;
(There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85504</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85504"/>
		<updated>2009-12-18T10:38:48Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
This is in part due to the pi bonding of the two fragments being on the same face of the molecule in the endo transition state, leaving sigma bonding MOs on the other face that can interact together (secondary orbital overlap). In the exo structure the pi and sigma bonding MOs cannot interact (they are now opposite each other), leading to a nodal plane. &lt;br /&gt;
&lt;br /&gt;
(There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85499</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85499"/>
		<updated>2009-12-18T10:34:14Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Regioselectivity of the Diels-Alder reaction */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. These were determined as above, by the TS (Berny) optimisation and frequency method (semi-empirical AM1 level; opt=noeigen, always calculate force constants), from an initial guess structure, based on the literature. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
(There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85498</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85498"/>
		<updated>2009-12-18T10:31:26Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|600 x 300 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
(There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3ptshomoscompsoo.jpg&amp;diff=85497</id>
		<title>File:Jr407m3ptshomoscompsoo.jpg</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3ptshomoscompsoo.jpg&amp;diff=85497"/>
		<updated>2009-12-18T10:31:06Z</updated>

		<summary type="html">&lt;p&gt;Jr407: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85496</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85496"/>
		<updated>2009-12-18T10:30:50Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Regioselectivity of the Diels-Alder reaction */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. In addition, the HOMO of the exo system has a node not present in the endo, as shown below; the endo benefits from a more extensive electron cloud conferring greater stability to the structure.  &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3ptshomoscompsoo.jpg|center|800 x 235 px|thumb|Transition state HOMOs.]]&lt;br /&gt;
&lt;br /&gt;
(There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85467</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85467"/>
		<updated>2009-12-18T10:09:44Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. The exo form is more strained most likely as a result of steric repulsion between the oxygen atoms on the carbonyl groups and the hydrogens on the bridging sp3 carbons, which have a through space separation of 2.69a.u.; this is in comparison to the endo form where the carbonyl oxygens are now in steric repulsion with a hydrogen on sp2 carbon (which has a planar configuration, increasing the O-H separation), the through space distance increasing to 3.31a.u.. &lt;br /&gt;
&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85464</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85464"/>
		<updated>2009-12-18T10:02:11Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
The relative energies of the transition structures (cyclohexa-1,3-diene reaction with maleic anhydride) are tabulated above (exo: -0.050420a.u.; endo: -0.051505a.u.), the endo being lower in energy and more stable by 0.68 kcal/mol. This confirms that under kinetic control the endo transition state will be reached first and the endo adduct dominates. &lt;br /&gt;
&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3paosinter.jpg&amp;diff=85463</id>
		<title>File:Jr407m3paosinter.jpg</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3paosinter.jpg&amp;diff=85463"/>
		<updated>2009-12-18T09:54:59Z</updated>

		<summary type="html">&lt;p&gt;Jr407: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85462</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85462"/>
		<updated>2009-12-18T09:54:44Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
[[Image:jr407m3paosinter.jpg|thumb|right|HOMO-LUMO interactions.]]&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
The representation of HOMO-LUMO interaction in terms of AOs is shown right.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85458</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85458"/>
		<updated>2009-12-18T09:50:14Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Optimising the transition structures */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level; TS (Berny)). The guess structure was achieved after using through space fragment separations of 2.2a.u. and 1.5a.u., which resulted in returning separate reactants and the product respectively - adjusting to 2.00a.u. allowed for a transition state. Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85457</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85457"/>
		<updated>2009-12-18T09:33:07Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; thus non-bonded carbons must be 3.4Å apart, the through space separation is 2.12Å confirming a transition structure with partial bonds. &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85456</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85456"/>
		<updated>2009-12-18T09:31:53Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; confirming that steric repulsions will be present.  &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|800 x 249 px|thumb|Forming the transition state HOMO / geometry analysis.]]&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3phomoforming2exts.jpg&amp;diff=85455</id>
		<title>File:Jr407m3phomoforming2exts.jpg</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3phomoforming2exts.jpg&amp;diff=85455"/>
		<updated>2009-12-18T09:31:16Z</updated>

		<summary type="html">&lt;p&gt;Jr407: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85454</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85454"/>
		<updated>2009-12-18T09:31:09Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; confirming that steric repulsions will be present.  &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoforming2exts.jpg|center|600 x 300 px|thumb|Forming the transition state HOMO.]]&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85449</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85449"/>
		<updated>2009-12-18T09:19:36Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;Cambridge Crystallographic Data Centre: http://www.ccdc.cam.ac.uk/products/csd/radii/table.php4&amp;lt;/ref&amp;gt; confirming that steric repulsions will be present.  &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoformingexts.jpg|center|600 x 300 px|thumb|Forming the transition state HOMO.]]&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85448</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85448"/>
		<updated>2009-12-18T09:11:11Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;DOI: 10.1021/j100785a001&amp;lt;/ref&amp;gt; confirming that steric repulsions will be present.  &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoformingexts.jpg|center|600 x 300 px|thumb|Forming the transition state HOMO.]]&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3phomoformingexts.jpg&amp;diff=85447</id>
		<title>File:Jr407m3phomoformingexts.jpg</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3phomoformingexts.jpg&amp;diff=85447"/>
		<updated>2009-12-18T09:10:46Z</updated>

		<summary type="html">&lt;p&gt;Jr407: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85446</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85446"/>
		<updated>2009-12-18T09:10:20Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;DOI: 10.1021/j100785a001&amp;lt;/ref&amp;gt; confirming that steric repulsions will be present.  &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO, as shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3phomoformingexts.jpg|center|800 x 235 px|thumb|Forming the transition state HOMO.]]&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3pcisbutMOs2.jpg&amp;diff=85444</id>
		<title>File:Jr407m3pcisbutMOs2.jpg</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3pcisbutMOs2.jpg&amp;diff=85444"/>
		<updated>2009-12-18T08:59:42Z</updated>

		<summary type="html">&lt;p&gt;Jr407: MOs&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;MOs&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85443</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85443"/>
		<updated>2009-12-18T08:59:23Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* MO analysis of cis-butadiene */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs2.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;DOI: 10.1021/j100785a001&amp;lt;/ref&amp;gt; confirming that steric repulsions will be present.  &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85442</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85442"/>
		<updated>2009-12-18T08:53:15Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* MO analysis of cis-butadiene */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4293   -0.3433   -0.2361   -0.1031   -0.0005    0.9267&lt;br /&gt;
 Low frequencies ---    2.5946  312.4390  485.2250&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134552&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.109172&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;DOI: 10.1021/j100785a001&amp;lt;/ref&amp;gt; confirming that steric repulsions will be present.  &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85347</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85347"/>
		<updated>2009-12-17T19:06:28Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4465   -5.9826   -2.0934   -0.0224    0.0035    0.1061&lt;br /&gt;
 Low frequencies ---    6.5194  312.6368  485.2126&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134553&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.108518&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;DOI: 10.1021/j100785a001&amp;lt;/ref&amp;gt; confirming that steric repulsions will be present.  &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
The HOMO of the transition structure is shown above, being anti-symmetric (a); the HOMO of cis-butadiene interacts with the LUMO of ethylene to form the transition state HOMO.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85346</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85346"/>
		<updated>2009-12-17T19:03:53Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4465   -5.9826   -2.0934   -0.0224    0.0035    0.1061&lt;br /&gt;
 Low frequencies ---    6.5194  312.6368  485.2126&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134553&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.108518&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;DOI: 10.1021/j100785a001&amp;lt;/ref&amp;gt; confirming that steric repulsions will be present.  &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. Below this the lowest real vibration is observed, a twisting of the dieneophile fragment over the diene, this is unlikely to correspond to a reaction path, as it does not bring the fragments closer together.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Is the HOMO at the transition structure s or a?&lt;br /&gt;
&lt;br /&gt;
Which MOs of butadiene and ethylene have been used to form this MO? Explain why the reaction is allowed.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3pts1viblow.jpg&amp;diff=85345</id>
		<title>File:Jr407m3pts1viblow.jpg</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Jr407m3pts1viblow.jpg&amp;diff=85345"/>
		<updated>2009-12-17T19:02:21Z</updated>

		<summary type="html">&lt;p&gt;Jr407: Lowest real vibration.&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Lowest real vibration.&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85344</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85344"/>
		<updated>2009-12-17T19:01:18Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Optimising the transition structures */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4465   -5.9826   -2.0934   -0.0224    0.0035    0.1061&lt;br /&gt;
 Low frequencies ---    6.5194  312.6368  485.2126&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134553&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.108518&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1viblow.jpg|right|200 x 200 px|thumb|Lowest real vibration.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;DOI: 10.1021/j100785a001&amp;lt;/ref&amp;gt; confirming that steric repulsions will be present.  &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Illustrate the vibration that corresponds to the reaction path at the transition state.  Is the formation of the two bonds synchronous or asynchronous? How does this compare with the lowest positive frequency?&lt;br /&gt;
&lt;br /&gt;
Is the HOMO at the transition structure s or a?&lt;br /&gt;
&lt;br /&gt;
Which MOs of butadiene and ethylene have been used to form this MO? Explain why the reaction is allowed.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85339</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85339"/>
		<updated>2009-12-17T18:55:16Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4465   -5.9826   -2.0934   -0.0224    0.0035    0.1061&lt;br /&gt;
 Low frequencies ---    6.5194  312.6368  485.2126&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134553&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.108518&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;DOI: 10.1021/j100785a001&amp;lt;/ref&amp;gt; confirming that steric repulsions will be present.  &lt;br /&gt;
&lt;br /&gt;
The vibration corresponding to the reaction path at the transition state is shown right - as discussed above - representing synchronous formation of the two bonds. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Illustrate the vibration that corresponds to the reaction path at the transition state.  Is the formation of the two bonds synchronous or asynchronous? How does this compare with the lowest positive frequency?&lt;br /&gt;
&lt;br /&gt;
Is the HOMO at the transition structure s or a?&lt;br /&gt;
&lt;br /&gt;
Which MOs of butadiene and ethylene have been used to form this MO? Explain why the reaction is allowed.&lt;br /&gt;
&lt;br /&gt;
==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
&lt;br /&gt;
The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
&lt;br /&gt;
The energies of the endo transition state are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
&lt;br /&gt;
And the principal MOs illustrated below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
&lt;br /&gt;
And of the exo transition state: &lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
&lt;br /&gt;
Again the principal MOs are again shown below. &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
&lt;br /&gt;
The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
&lt;br /&gt;
*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
&lt;br /&gt;
===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
&lt;br /&gt;
Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
&lt;br /&gt;
Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
&lt;br /&gt;
==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
&lt;br /&gt;
Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85338</id>
		<title>Rep:Namespace:jr4073PROJECT</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=Rep:Namespace:jr4073PROJECT&amp;diff=85338"/>
		<updated>2009-12-17T18:52:15Z</updated>

		<summary type="html">&lt;p&gt;Jr407: /* Discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:jr407comptransitionstatescycloadd.jpg|thumb|left|200px|An example Diels-Alder cycloaddition (Michigan State University).]]&lt;br /&gt;
&#039;&#039;&#039;Modelling Techniques &amp;amp; Calculations&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
The computational models may be built from ChemDraw structural drawings, which convert to 3D structures in Chem3D, or by direct modelling in GaussView. Optimisations may be run by MM2 (molecular mechanics) or PM6 (semi-empirical molecular orbital theory) in Chem3D. The principale method here is the use of Gaussian to run molecular orbital-based quantum calculations - numerically solving the Schroedinger equation - giving a more accurate result.  &lt;br /&gt;
&lt;br /&gt;
=&#039;&#039;&#039;The Diels-Alder Cycloaddition&#039;&#039;&#039;=&lt;br /&gt;
A Diels Alder reaction is a pericyclic reaction between a diene and a dieneophile, the π orbitals of the two species interacting to form new σ bonds. For such a reaction to be allowed the HOMO of one reactant must interact with the LUMO of the other (forming two new MOs, one bonding and one anti-bonding). Furthermore, for a reaction there must be good orbital overlap; differing symmetry makes this impossible and the reaction forbidden. &lt;br /&gt;
&lt;br /&gt;
The addition of substituents (with π orbitals) to the dieneophile stabilises the regiochemistry of the addition by interacting with the new double bond on the product (known as secondary orbital effects). &lt;br /&gt;
&lt;br /&gt;
The transition structures for Diels-Alder cycloadditions - with both substituted and unsubstituted dieneophiles - are determined, considering the MOs also, to predicted reactivity. Under kinetic control the product with the lower energy transition state dominates, as illustrated below.&lt;br /&gt;
&lt;br /&gt;
[[Image:Kineticcarcrash.jpg|center|400 x 135 px|thumb|Transition state theory: under kinetic control product B dominates, despite the greater stability of product A.]]&lt;br /&gt;
&lt;br /&gt;
==Prototypical Diels-Alder cycloaddition: ethylene + cis-butadiene==&lt;br /&gt;
[[Image:jr407m3ptypical.jpg|thumb|right|Prototypical Diels-Alder cycloaddition.]]&lt;br /&gt;
&lt;br /&gt;
The reaction scheme between ethylene and butadiene to give cyclohexene via a Diels-Alder cycloaddition is shown right. The way in which the reactants come together in the transition state is governed by π orbital interactions, principally the HOMO and LUMO of each. In this case there is a [4s + 2s] addition (this reflects the number of π orbitals present). The MO interactions are considered in more detail below, with the transition states of such cycloadditions to predict reactivity.&lt;br /&gt;
&lt;br /&gt;
===MO analysis of cis-butadiene===&lt;br /&gt;
[[Image:jr407m3pcisbutopt.jpg|thumb|right|Optimised cis-butadiene.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;Cisbutadieneopt2JMOL.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Cis-butadiene - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pcisbutmosener.jpg|thumb|right|Cis-butadiene MO energies.]]&lt;br /&gt;
&lt;br /&gt;
Cis-butadiene has been geometry optimised (AM1 level) giving the structure shown right (click to enlarge &amp;amp; click button for 3D JMol). Optimisation is confirmed in the .log output file and by frequency (vibrational) analysis - there are no imaginary frequencies and thus a global minima has been achieved:&lt;br /&gt;
&lt;br /&gt;
Optimization completed.&lt;br /&gt;
    -- Stationary point found.&lt;br /&gt;
&lt;br /&gt;
 Low frequencies ---  -39.4465   -5.9826   -2.0934   -0.0224    0.0035    0.1061&lt;br /&gt;
 Low frequencies ---    6.5194  312.6368  485.2126&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.134553&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.138573&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.139517&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.108518&lt;br /&gt;
&lt;br /&gt;
The HOMO and LUMO are shown below with their symmetry relative to a vertical plane (sketched). &lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pcisbutMOs.jpg|center|800 x 235 px|thumb|MO analysis of cis-butadiene.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO is anti-symmetric and the LUMO symmetric, and the number of nodes increases with the energy of the MO (energies are shown right).&lt;br /&gt;
&lt;br /&gt;
===Optimising the transition structures===&lt;br /&gt;
[[Image:jr407m3penvelopts.jpg|right|200 x 200 px|thumb|Envelope structure transition state.]]&lt;br /&gt;
[[Image:jr407m3pts1.jpg|thumb|right|Optimised transition state.|&amp;lt;jmol&amp;gt;&lt;br /&gt;
&amp;lt;jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;uploadedFileContents&amp;gt;TRANSITIONSTATEOPTjmol.mol&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;text&amp;gt;Transition state - JMol&amp;lt;/text&amp;gt;&lt;br /&gt;
&amp;lt;/jmolAppletButton&amp;gt;&lt;br /&gt;
&amp;lt;/jmol&amp;gt;]]&lt;br /&gt;
[[Image:jr407m3pts1vib.jpg|right|200 x 200 px|thumb|Imaginary vibration corresponding to reaction.]]&lt;br /&gt;
[[Image:jr407m3pts1moenergies.jpg|right|200 x 200 px|thumb|Relative energies of TS MOs.]]&lt;br /&gt;
The transition state for the reaction between ethylene and cis-butadiene is known to have an envelope type structure to maximise the π orbital overlap between the reactants. The transition state structure has been optimised from an initial guess, shown right (AM1 level). Simultaneous frequency analysis confirms this to be a transition state by the presence of an imaginary vibration:&lt;br /&gt;
&lt;br /&gt;
 Low frequencies --- -956.1133   -3.7882   -2.8348   -0.4038   -0.0031    0.0485&lt;br /&gt;
 Low frequencies ---    0.0842  147.2135  246.6165&lt;br /&gt;
&lt;br /&gt;
The thermal energies of the system are noted:&lt;br /&gt;
&lt;br /&gt;
 Sum of electronic and zero-point Energies=              0.253277&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.259454&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.260398&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.224017&lt;br /&gt;
&lt;br /&gt;
Animation of the imaginary vibration corresponds to the pericyclic reaction as the two fragments come together (shown right - click to enlarge).&lt;br /&gt;
&lt;br /&gt;
The principal MOs of the transition state and their symmetry are described below, their relative energies being plotted right.&lt;br /&gt;
&lt;br /&gt;
[[Image:jr407m3pts1aMOs.jpg|center|800 x 235 px|thumb|MO analysis of the transition state.]]&lt;br /&gt;
&lt;br /&gt;
Notably the HOMO has three nodes creating six clouds of electron density in an antisymmetric array about the plane shown.&lt;br /&gt;
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===Discussion===&lt;br /&gt;
Typically sp3 bonded carbon has a C-C bondlength of 1.54Å, and sp2 carbon a C=C bondlength of 1.34Å.&amp;lt;ref&amp;gt; Atkins, P., and de Paula, J., Physical Chemistry, (8th Ed.), Oxford: Oxford University Press, 2006&amp;lt;/ref&amp;gt; The observed bond lengths are intermittant between the two, indicative of a transition state with delocalised bonding. In addition, carbon has an atomic van der Waals radius of 1.70Å.&amp;lt;ref&amp;gt;DOI: 10.1021/j100785a001&amp;lt;/ref&amp;gt; confirming that steric repulsions will be present.  &lt;br /&gt;
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Illustrate the vibration that corresponds to the reaction path at the transition state.  Is the formation of the two bonds synchronous or asynchronous? How does this compare with the lowest positive frequency?&lt;br /&gt;
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Is the HOMO at the transition structure s or a?&lt;br /&gt;
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Which MOs of butadiene and ethylene have been used to form this MO? Explain why the reaction is allowed.&lt;br /&gt;
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==Regioselectivity of the Diels-Alder reaction==&lt;br /&gt;
[[Image:jr407m3pregioscheme.jpg|thumb|right|Regioselectivity: reaction scheme.]]&lt;br /&gt;
It is known that cyclohexa-1,3-diene reacts with maleic anhydride giving the endo adduct as the major product - this is supposed to be a result of kinetic control and the exo transition state being higher in energy. The reaction is shown right. &lt;br /&gt;
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The transition structures leading to both products are shown below, with their corresponding energies below and C-C &#039;bond&#039; distances tabulated. &lt;br /&gt;
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[[Image:jr407m3pexertab11.jpg|center|800 x 235 px|thumb|Geometry analysis of transition states.]]&lt;br /&gt;
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The energies of the endo transition state are noted:&lt;br /&gt;
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 Sum of electronic and zero-point Energies=              0.133494&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.143683&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.144628&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.097351&lt;br /&gt;
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And the principal MOs illustrated below. &lt;br /&gt;
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[[Image:jr407m3pendoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the endo transition state.]]&lt;br /&gt;
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And of the exo transition state: &lt;br /&gt;
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 Sum of electronic and zero-point Energies=              0.134881&lt;br /&gt;
 Sum of electronic and thermal Energies=                 0.144882&lt;br /&gt;
 Sum of electronic and thermal Enthalpies=               0.145827&lt;br /&gt;
 Sum of electronic and thermal Free Energies=            0.099117&lt;br /&gt;
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Again the principal MOs are again shown below. &lt;br /&gt;
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[[Image:jr407m3pexoMOstab2.jpg|center|800 x 235 px|thumb|Principal MOs of the exo transition state.]]&lt;br /&gt;
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The sum of free energies (and all other thermal chemistry properties listed) for the endo transition state are lower than for the exo; the C-C &#039;bond&#039; distances are highly similar in both cases, as is the general shape of the MOs, however these are much lower again for the endo. This confirms that under kinetic control the endo adduct will dominate as the precursing transition state is reached sooner.  &lt;br /&gt;
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*What can you conclude about the so called “secondary orbital overlap effect”?&lt;br /&gt;
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===Discussion===&lt;br /&gt;
For the cyclohexa-1,3-diene reaction with maleic anhydride:&lt;br /&gt;
Give the relative energies of the exo and endo transition structures. Comment on the structural difference between the endo and exo form. Why do you think that the exo form could be more strained? Examine carefully the nodal properties of the HOMO between the -(C=O)-O-(C=O)- fragment and the remainder of the system. What can you conclude about the so called “secondary orbital overlap effect”? (There is some discussion of this in Ian Fleming&#039;s book &#039;Frontier Orbitals and Organic Chemical Reactions&#039;).&lt;br /&gt;
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Further discussion:&lt;br /&gt;
What effects have been neglected in these calculations of Diels Alder transition states?&lt;br /&gt;
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Look at published examples and investigate further if you have time. (e.g. DOI:10.1021/jo0348827 )&lt;br /&gt;
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==Error analysis...==&lt;br /&gt;
Calculated energies are accurate to ~10kJ/mol - 0.003809a.u. - and are thus reported to 0.01a.u.; dipole moments are accurate to 0.01 Debye, and frequencies reported to 1cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; (typically 10% error), likewise intensities (infrared) are given as whole numbers; bond distances are accurate to 0.01a.u. and angles to 0.1deg. &lt;br /&gt;
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Notably energies &#039;&#039;between&#039;&#039; molecules should only be considered on a relative (kJ/mol; not absolute!) level; absolute values are noted for reproducibility only (a.u.), and consistency is paramount for comparison (basis set, method, details). &lt;br /&gt;
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==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
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==External links==&lt;br /&gt;
* [Michigan State University - Reactions of Alkenes: http://www.cem.msu.edu/~reusch/VirtualText/addene2.htm]&lt;br /&gt;
* [Chemistry SCAN Link: https://scanweb.cc.imperial.ac.uk/uportal2/]&lt;br /&gt;
* [Illustration of vibrational mode categories: http://en.wikipedia.org/wiki/Infrared_spectroscopy]&lt;br /&gt;
* [Online symmetry point group flow chart: http://capsicum.me.utexas.edu/ChE386K/Images/point_group_flowchart_shriver.jpg]&lt;/div&gt;</summary>
		<author><name>Jr407</name></author>
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