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Rep:Mod:JS6313 TS

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Introduction

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Units

In this article, energies are given in atomic units of energy, a.u,; 1 a.u. is equivalent to 1 hartree which is defined as Rhc, where R is the Rydberg constant, h is Planck's constant and c is the speed of light in a vacuum. This comes out as 1 a.u. = 4.359 744 650 x 10-18 J.[1]

Cope Rearrangement (Tutorial)

Optimisations in this section have been carried out using the Hartree-Fock method and the 3-21G basis set. The first two calculations were for 1,5-hexadiene in the anti and gauche conformations, both of which were found to have C1 symmetries. As expected, the anti conformation was found to have a slightly lower energy, which can be attributed to steric clashing between carbons 2 and 4.

The conformation which would be expected to be the lowest in energy, taking into account only sterics, is anti when viewed along carbons 3 and 4. This turns out not to be the case; in fact, it is when the substituents on these carbons are in a gauche to each other.

Processed Model Symmetry Energy (a. u.) Relative Energy (kcal/mol) Manual Wiki Structure
Chair transition state after 'derivative' ModRedundant parameters
Chair transition state after 'derivative' ModRedundant parameters
C1 -231.69097049 1.07 anti4
Chair transition state after 'derivative' ModRedundant parameters
Chair transition state after 'derivative' ModRedundant parameters
C2 -231.69166702 0.63 gauche2
Chair transition state after 'derivative' ModRedundant parameters
Chair transition state after 'derivative' ModRedundant parameters
C1 -231.69266119 0.00 gauche3
Chair transition state after 'derivative' ModRedundant parameters
Chair transition state after 'derivative' ModRedundant parameters
Ci -231.69253528 0.08 anti2

The anti2 conformation only changes slightly when run at the DFT level of theory and a 6-31G(d) basis set. All angles are within 0.6° of their corresponding angles on each basis set. These are the various values found in the output file of the optimised and frequency analysed anti2 conformer:

Value Energy (a.u.)
Sum of electronic and zero-point energies -234.469214
Sum of electronic and thermal Energies -234.461866
Sum of electronic and thermal Enthalpies -234.460922
Sum of electronic and thermal Free Energies -234.500798

Optimising the "Chair" and "Boat" Transition Structures

The first guess at a chair transition state for two C3H5 fragments gave the expected singular imaginary frequency at -818 cm-1; this shows that the optimised structure

Optimised chair transition state

is at a potential energy maximum saddle point. Any disturbance from this state would result in either product or back to reactants.

Fixing the forming/breaking bond lengths at 2.2 Å ran as expected; the terminal distances were in fact 2.2 Å and 2.27 Å. Upon fixing the hessian and using 'derivative' as opposed to 'add', the structure did not visibly change but the bond angles changed to 2.21 Å and 2.25 Å.

Chair transition state after 'derivative' ModRedundant parameters
Boat transition state optimised with TS(QST2). Bond lengths for 'terminal' carbon-carbon interractions are both 2.14 Å. It has one imaginary frequency at -840 cm-1 which is consistent with a transition state.

Diers-Alder Cycloaddition

Optimised butadiene (semi-empirical)
Optimised butadiene (semi-empirical)
Optimised butadiene HOMO and LUMO (semi-empirical)
Optimised butadiene HOMO and LUMO (semi-empirical)

The HOMOs shown here are antisymmetric with respect to the plane of the cis-butadiene molecule.

Optimised ethylene and budadiene approaches
  1. http://physics.nist.gov/cgi-bin/cuu/Value?hr