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Unit II β Bonding Theories Β· Molecular Orbital Theory
MOT treats electrons as belonging to the whole molecule via molecular orbitals; it explains Oβ's paramagnetism, bond order and magnetic character.
Two AOs of same symmetry combine to give one bonding MO (lower energy, electron density between nuclei) and one antibonding MO Ο*/Ο* (higher energy, node between nuclei). The number of MOs equals the number of AOs combined.
For second-period homonuclear diatomics (Liβ to Nβ): Ο1s < Ο*1s < Ο2s < Ο*2s < Ο2pz < Ο2px=Ο2py < Ο*2px=Ο*2py < Ο*2pz. From Oβ onwards, Ο2pz drops below Ο2px/Ο2py because of s-p mixing effects. Electrons fill in by Hund's rule.
Bond order = (bonding β antibonding)/2. A fractional or non-integer order plus unpaired electrons explains properties.
| Molecule | Bond order | Magnetic nature |
|---|---|---|
| Bβ | 1 | Paramagnetic (2 unpaired) |
| Cβ | 2 | Diamagnetic |
| Nβ | 3 | Diamagnetic |
| Oβ | 2 | Paramagnetic (2 unpaired) |
| Fβ | 1 | Diamagnetic |
| CO | 3 | Diamagnetic (isoelectronic Nβ) |
| NO | 2.5 | Paramagnetic |
MO = bonding (lower) + antibonding (higher). Bond order = (Nb β Na)/2. Unpaired electrons β paramagnetism. Recall Oβ, Nβ, NO, CO, Bβ, Cβ, Fβ.