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Physical chemistry     280


                         Homonuclear second row diatomic molecules

        Diatomic molecules composed of identical atoms N 2 and O 2, for example, are referred to
        as homonuclear diatomic molecules. In the second and subsequent rows of the periodic
        table, the bonding interactions involve both p and s orbital interactions. By convention,
        the bonding axis is taken to be the z axis and the linear combinations of the p z orbitals
        differ from those of the p x and p y orbitals.
           The lobes of the atomic p z orbitals interact directly and relatively strongly along the
        bonding axis to form molecular bonding and antibonding a orbital combinations.  The
        linear combinations of the p x and p y orbitals on the other hand give rise to two bonding
        and antibonding  π orbital combinations  (Fig. 3). The overlap of  the  p x and of the  p y
        orbitals is smaller than that of the p z orbitals, and this is reflected in the energy of the a
        bond which is lower than that of the two π bonds. The two π bonds are of equal energy
        and are said to be degenerate.
           Core atomic  orbitals do not make a significant contribution to the bonding in a
        molecule for two reasons. Firstly, there is no significant overlap of these orbitals, and the
        energy of the bonding orbitals is not significantly lower than the  atomic  orbitals,  and
        secondly, each pair of bonding and antibonding is fully occupied, leaving no net bonding
        contribution.
           The molecular orbital diagram for a second row diatomic, O 2, is shown in Fig. 3, with
        eight 2p electrons occupying the two degenerate bonding π-orbitals, the bonding σ-orbital
        and two degenerate π* orbitals to give a double bond overall.
           The σ bonding and antibonding molecular orbitals derived from the 1s and 2s atomic
        orbitals are fully occupied and so have no net bonding effect. In oxygen, the two highest
        energy electrons are placed separately into the π x* and π y* orbitals to give two unpaired
        electrons, which also confer oxygen with significant paramagnetism.
           As  the molecular orbitals are qualitatively unchanged, the same molecular orbital
        diagram may be used to describe any second row diatomic molecule or ion, by simply
        entering  the correct number of electrons.  However, detailed analysis reveals the
        importance of including all the atomic orbitals when generating the linear combination of
        orbitals. The narrow energy gap between the 2s and 2p orbitals in the early part of the
        second row leads to mixing of the 2s atomic orbitals with the 2p z orbitals. This raises the
        energy of the 2p z generated  σ orbitals, and lowers the  energy  of  the  2s generated  σ*
        orbital, so that the highest occupied π and σ bonding orbitals exchange positions between
        nitrogen and oxygen (Fig. 4).
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