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Polyatomic molecules - Cobalt

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The set of linear equations reads<br />

C ( α− E)<br />

+ C β = 0<br />

11<br />

12<br />

C β + C ( α− E)<br />

+ C β =0<br />

11 12<br />

13<br />

C<br />

12<br />

β<br />

+C<br />

12<br />

( α− E)<br />

= 0<br />

We get<br />

1 1 1<br />

1 1<br />

1 1 1<br />

ψ = ϕ + ϕ + ϕ ; ψ = ϕ − ϕ ; ψ = ϕ − ϕ + ϕ<br />

2 2 2<br />

2 2 2 2 2<br />

1 1 2 3 2 1 3 3 1 2 3<br />

3. (a) In the ' free electron molecular orbital' (FEMO) theory, the electrons<br />

in a conjugated molecule are treated as independent particles in a box<br />

of length L . Sketch the form of the two occupied orbitals in butadiene, predicted<br />

by this model and predict the minimum excitation energy of the molecule.<br />

Comments on the relation to the π - orbitals obtained in Atkins. What are the<br />

similarities and the differences. What are the differences between the spacing<br />

of the orbitals in the two methods.<br />

Answer<br />

2 2<br />

n h<br />

2 n x<br />

En = =<br />

⎛ π<br />

, n = 1,2,3....... and ψ sin<br />

⎞<br />

2<br />

n<br />

8mL<br />

L ⎝ L ⎠<br />

The Orbitals of the three first levels are given by :<br />

FMO<br />

Huckel<br />

E 3 =<br />

9h 2<br />

8mL 2 ,<br />

α−.62β<br />

4 h 2<br />

E 2 =<br />

8mL 2 ,<br />

α+.62β<br />

E 1 =<br />

h 2<br />

8mL 2 ,<br />

α+1.62β

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