Explicit Forms

So what are the combinations of hydrogen orbitals which form the A1 and B1 molecular orbitals? We can work this out by a process very similar to the one we used to generate the reducible representation in the first place.
Let us consider the two s-orbitals on the hydrogen atoms, and label them as s1 and s2. We then look at what happens to them under each transformation.


2 H s-orbitals

C2v E C2 sv(xz) sv(yz)
s1 s1 s2 s1 s2

i.e. under the identity operation, s1 remains in the same place. Under C2 rotation, it exchanges places with s2, etc.

To generate the combination of orbitals which has A1 symmetry, we multiply by the A1 irreducible representation:

C2v E C2 sv(xz) sv(yz)
A1 1 1 1 1
s1 s1 s2 s1 s2

So for the sigma-bond of A1 symmetry, s(A1),

s(A1) = 1 x s1 + 1 x s2 + 1 x s1 + 1 x s2
= 2 x s1 + 2 x s2

The result of this must be normalised. To do this we take the square rot of the sum of the squares of the coefficients, and divide the explicit form by this, i.e.

sum = 22 + 22 = 8
Ö8 = 2Ö2
s(A1) = 2 x s1 + 2 x s2
2Ö2
= 1 (s1 + s2)
Ö2

The B1 combination can be found by a similar process:

C2v E C2 sv(xz) sv(yz)
B1 1 -1 1 -1
s1 s1 s2 s1 s2

Hence,

s(B1) = 1 x s1 - 1 x s2 + 1 x s1 - 1 x s2
= 2 x s1 - 2 x s2

and after normalisation,

s(B1) = 1 (s1 - s2)
Ö2


We can now draw the orbitals which are used for the complete molecular orbital.
The A1 bonding molecular orbital:

A1 bonding M.O.

Note that both the hydrogen atomic orbitals have the same sign.
The A1 antibonding molecular orbital:

A1 antibonding M.O.

Note that the hydrogen orbitals and the oxygen hybrid orbital have opposite signs.

The B1 bonding molecular orbital:

B1 bonding M.O.

Note that the hydrogen orbitals have opposite signs, and that there is a good bonding overlap with the oxygen px orbital, which is of B1 symmetry.
The B1 antibonding molecular orbital:

B1 antibonding M.O.

This is an antibonding interaction with the oxygen px orbital.

Such a molecular orbital is called a symmetry-adapted linear combination or SALC.

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Author: Mike Hammond, University of Sheffield Department of Chemistry.
Last Modified: 11th April 2000.