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Mini Paper: Orbital Symmetry Rules for Unimolecular Reactions 
Ralph G. Pearson, JACS, 94:24. 1972 
__________________________________________________________________________________ 
To predict the course of a reaction Perturbation theory has been applied rigorously, here the author has come up with simple symmetry rules, which accounted for several unimolecular reactions shown here. 
To start, The Transition density: changed electron density for the mixing of ground and excited state wave function in the course of reaction, ρ, is proportional to Фi x Фf where Фi is initial and Фf is final MO occupied. So reaction path will be chosen by the reactant(s) in where the symmetry of the reaction coordinate will be same as the Фi x Фf. After reaction begins Q must be totally symmetric. 
For Unimolecular reactions this has been discussed as follows: 
H2 → 2H 
The valence shell orbitals are of σ g (b.) and σu (a. b.) symmetry. The reaction coordinate is totally symmetric, or Σg+. Dissociation must involve movement of electrons from the σ g to σ u orbitals. The symmetry rule then requires that the excited state which mixes into the ground state is the doubly excited configuration, (σ u)2. 
CH4 → CH3 + H 
Requires a Tz vibration to break the Td point group. This can occur most easily by a (t2) → (a1*) excitation. After a short extension of the carbon-hydrogen bond, the point group becomes C3v , the reaction coordinate becomes A1, and the remaining process is that for a heteronuclear diatomic molecule. 
SF4 → SF2 + F2 -allowed 
SO2F2 → SO2 + F2 -forbidden 
The S-F bonds to be broken in both cases are of a1 and b2, symmetry in the C2v point group. The F-F bond to be made is of a1 symmetry. In the case of SF4, the remaining new bonds are actually antibonding, since a π* orbital of b2 symmetry is filled. 
In the case of SO2, which has two fewer electrons that SF2, the new orbital that is filled is either an antibonding σ * orbital of al symmetry, or a π nonbonding MO of a2 symmetry. These two orbitals appear to have rather similar energies. At any rate, normally there are no electrons in the higher energy π* orbital of b2, symmetry. Since under the influence of an A1 perturbation (the changing reaction coordinate), electrons cannot move from a b2, orbital (S-F bonding) into either an a1* or a2* orbital. The symmetries of the bonds and the reaction coordinate do not match up. Hence the reaction is forbidden.
C6H10 → C4H6 + C2H4 
the bonds that are broken (the 3-4 π bond and the 1-2 and 5-6 σ bonds) are of 2A’ + A” symmetry. The bonds to be made (the 1-6, 4-5, and 2-3 π bonds) are of the same symmetry. 
They concluded, the rule that a reaction is allowed, if the symmetries of the bonds that are made match up with the symmetries of the bonds that are broken. 
__________________________________________________________________________________ 
-Sujoy Saha 
BS-MS 
20101095

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Orbital Symmetry Rules for Unimolecular Reactions

  • 1. Mini Paper: Orbital Symmetry Rules for Unimolecular Reactions Ralph G. Pearson, JACS, 94:24. 1972 __________________________________________________________________________________ To predict the course of a reaction Perturbation theory has been applied rigorously, here the author has come up with simple symmetry rules, which accounted for several unimolecular reactions shown here. To start, The Transition density: changed electron density for the mixing of ground and excited state wave function in the course of reaction, ρ, is proportional to Фi x Фf where Фi is initial and Фf is final MO occupied. So reaction path will be chosen by the reactant(s) in where the symmetry of the reaction coordinate will be same as the Фi x Фf. After reaction begins Q must be totally symmetric. For Unimolecular reactions this has been discussed as follows: H2 → 2H The valence shell orbitals are of σ g (b.) and σu (a. b.) symmetry. The reaction coordinate is totally symmetric, or Σg+. Dissociation must involve movement of electrons from the σ g to σ u orbitals. The symmetry rule then requires that the excited state which mixes into the ground state is the doubly excited configuration, (σ u)2. CH4 → CH3 + H Requires a Tz vibration to break the Td point group. This can occur most easily by a (t2) → (a1*) excitation. After a short extension of the carbon-hydrogen bond, the point group becomes C3v , the reaction coordinate becomes A1, and the remaining process is that for a heteronuclear diatomic molecule. SF4 → SF2 + F2 -allowed SO2F2 → SO2 + F2 -forbidden The S-F bonds to be broken in both cases are of a1 and b2, symmetry in the C2v point group. The F-F bond to be made is of a1 symmetry. In the case of SF4, the remaining new bonds are actually antibonding, since a π* orbital of b2 symmetry is filled. In the case of SO2, which has two fewer electrons that SF2, the new orbital that is filled is either an antibonding σ * orbital of al symmetry, or a π nonbonding MO of a2 symmetry. These two orbitals appear to have rather similar energies. At any rate, normally there are no electrons in the higher energy π* orbital of b2, symmetry. Since under the influence of an A1 perturbation (the changing reaction coordinate), electrons cannot move from a b2, orbital (S-F bonding) into either an a1* or a2* orbital. The symmetries of the bonds and the reaction coordinate do not match up. Hence the reaction is forbidden.
  • 2. C6H10 → C4H6 + C2H4 the bonds that are broken (the 3-4 π bond and the 1-2 and 5-6 σ bonds) are of 2A’ + A” symmetry. The bonds to be made (the 1-6, 4-5, and 2-3 π bonds) are of the same symmetry. They concluded, the rule that a reaction is allowed, if the symmetries of the bonds that are made match up with the symmetries of the bonds that are broken. __________________________________________________________________________________ -Sujoy Saha BS-MS 20101095