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Contents
Module3:Transition states and reactivity
Introduction
The Cope Rearrangement of 1,5-hexadiene
The Cope rearrangement of 1,5-hexadiene is a typical [3,3]sigmatropic rearrangement. The mechanism of this reaction is generally believe to go trough 'chair' and 'boat' transition state(TS). During the tutorial, we built both transition structure and found their activation energies.
Reactants
| Conformer | Structure | Point Group | Energy/Hartrees HF/3-21G | Relative Energy/kcal/mol |
|---|---|---|---|---|
| gauche3 |
|
C1 | -231.692660 | 0.00 |
| anti2 |
|
Ci | -231.69253529 | 0.08 |
| anti3 |
|
C2h | -231.689069999 | 2.25 |
Chair and Boat Transition Structure
Chair Transition Structure
| Imaginary Frquency of chair TS |
|
Boat Transition Structure
| Imaginary Frquency of boat TS |
|
QTS2 is used to generated to transition structure form the structure of reactant and product. The numbering of atomic from atomic list must be keep the same order.
Intrinsic Reaction Coordinate
| IRC for the reaction | Energy plot for the IRC |
|
In this case, IRC is only running in one direction as the reaction is symmetric and the other direction will be exactly the same. Where as for the reaction is not symmetric, it is necessary to run the IRC in both direction(which is used in later past of this wiki page).
| At 298.15K | Chair-TS | Boat-TS | ||
|---|---|---|---|---|
| HF/3-21G | B3LYP/6-31G* | HF/3-21G | B3LYP/6-31G* | |
| Sum of electronic and zero-point Energies | -231.466714 | -234.411655 | -234.391626 | -234.427323 |
| Sum of electronic and thermal Energies | -231.461353 | -234.405192 | -231.450922 | -234.392570 |
| Sum of electronic and thermal Enthalpies | -231.602802 | -234.441291 | -231.444349 | -234.396006 |
| Sum of electronic and thermal Free Energies | -231.495222 | -231.466714 | -231.479768 | -234.461856 |
| At 0K | Chair-TS | Boat-TS | ||
|---|---|---|---|---|
| HF/3-21G | B3LYP/6-31G* | HF/3-21G | B3LYP/6-31G* | |
| Sum of electronic and zero-point Energies | -231.466714 | -234.411655 | -231.450922 | -234.398496 |
| Sum of electronic and thermal Energies | -231.466714 | -234.411655 | -231.450922 | -234.398496 |
| Sum of electronic and thermal Enthalpies | -231.466714 | -234.411655 | -231.450922 | -234.398496 |
| Sum of electronic and thermal Free Energies | -231.466714 | -234.411655 | -231.450922 | -234.398496 |
| HF/3-21G | B3LYP/6-31G* | |||||
|---|---|---|---|---|---|---|
| Electronic energy | Sum of electronic and zero-point energies | Sum of electronic and thermal energies | Electronic energy | Sum of electronic and zero-point energies | Sum of electronic and thermal energies | |
| at 0 K | at 298.15 K | at 0 K | at 298.15 K | |||
| Chair TS | -231.466714 | -231.466714 | -231.461353 | -234.54046002 | -234.411655 | -234.405192 |
| Boat TS | -231.60280239 | -231.450922 | -231.445294 | -234.54046002 | -234.398497 | -234.392570 |
| Reactant (anti2) | -231.692535 | -231.539539 | -231.532566 | -234.611710 | -234.469203 | -234.461856 |
Summary of activation energies (in kcal/mol)
| HF/3-21G | HF/3-21G | B3LYP/6-31G* | B3LYP/6-31G* | Expt. | |
| at 0 K | at 298.15 K | at 0 K | at 298.15 K | at 0 K | |
| ΔE (Chair) | 45.70 | 44.69 | 36.11 | 34.93 | 33.5 ± 0.5 |
| ΔE (Boat) | 55.61 | 54.76 | 44.37 | 43.48 | 44.7 ± 2.0 |
From the Activation energies that calculated above, the HF/21G optimisation result is less actuate than 6-31G* as the activation energy generated from 6-31G* is way closer in both case.
The Diels Aider Cycloaddition
Cis-butadiene and Ethene
| HOMO | LUMO | |
| butadiene | ||
| ethene |
(The butadiene structure in the figures above does not seem to be in a planar configuration, C2v, is that what you expected? João (talk) 12:30, 12 February 2015 (UTC)) As shown in the graph above, the HOMO and LUMO of cis-butadiene are both symmetrical to the mirror plane. The HOMO transition state is generate from LUMO of butadiene (S)and HOMO ethene(S). The LUMO of TS is generated from LUMO (S)of ditadiene and LUMO+1(AS). It is worth noticing that AS and S can generate symmetrical MO. (What is the overlap integral of a symmetric and an anti-symmetric orbital? Can they interact? João (talk) 12:30, 12 February 2015 (UTC))
| Imaginary Frquency of TS | HOMO of TS | LUMO of TS |
|
Endo vs Exo Diels-Alder Reaction
| Exo TS Imagery frequency | Endo TS Imagery frequency |
|
|
Exo product
| IRC of Exo product | Energy plot of IRC |
|
Endo Product
| IRC of Endo product | Energy plot of Endo IRC |
|
| electronic energy of starting point(hartree) | electronic energy of TS(hartree) | ΔE(hartree) | |
| exo | -605.651 | -605.610 | 0.041 |
| endo | -605.652 | -605.604 | 0.048 |
| activation energy to TS | kcal/mol |
| exo | 30.12 |
| endo | 25.73 |
The ICR calculation coverage backward to a local minimum on the both energy plot. Theoretically the backward reaction should not be converge as the reactants will have the minimum energy at infinity. This case we assume it is the energy of reactant as the molecule will approach to each other during the reaction. The different in energy of reactant and transition state is the activation energy.The calculation indicate that exo transition structure have a higher energy transition state(4.39 kcal/mol more than endo). As we know the reaction is driven by kinetics (Doesn't this depend on reaction conditions? What happens at high temperatures? João (talk) 12:30, 12 February 2015 (UTC)), the major product will endo-prodoct as it has a lower energy transition state.
| Endo | Exo | |
| LUMO | ||
| HOMO |
From the molecular orbital of Endo and Exo TS, It is important to see that in the HOMO of Endo-TS the Π orbital on oxygen in -(C=O)-O-(C=O)- fragment can interact and donating electron to the Π* orbital of conjugate double bond orbital in cyclohexa-1,3-diene shown in the LUMO of Exo-TS. This orbital contribution will lower down the overall electronic energy of Endo-TS. This secondary orbital overlap effect is consider to be the main contribution to the lower energy Transition state of endo-product. Where as for the Exo-Ts, there is effect is hard to observe.







