Page 291 - Instant notes
P. 291

H4
                  MOLECULAR ORBITAL THEORY OF
                         DIATOMIC MOLECULES II



        Key Notes
                                Molecular orbital energy levels may be represented by a
                                molecular orbital energy level diagram, which illustrates the
                                relative energy of the molecular and atomic orbitals, and their
                                relationship. The bonding molecular orbital is of lower energy
                                than that of the separate atomic orbitals, and the converse is true
                                for the antibonding orbital. The available electrons are placed in
                                pairs into the molecular orbitals, with the lowest energy
                                molecular orbitals being filled first. In the hydrogen molecule,
                                both electrons occupy the bonding molecular orbital, giving an
                                overall bonding interaction. In He 2 , two electrons occupy each of
                                the σ and σ* orbitals, giving no net bonding.
                                In second row diatomic molecules, linear combinations of the p
                                orbitals give both a σ orbital and two degenerate π orbitals. As
                                the molecular orbitals are qualitatively unchanged for the second
                                row diatomic molecules, the same molecular orbital diagram may
                                be used by entering the correct number of electrons. Detailed
                                analysis reveals that the highest occupied π and σ orbitals
                                exchange positions between the elements nitrogen and oxygen.
                                Core orbitals do not make a significant contribution to the
                                bonding, as each pair of bonding and antibonding orbitals is fully
                                occupied, leaving no net bonding contribution.
                                Molecular orbitals in homonuclear molecules may be described
                                in terms of their symmetry with respect to a point of inversion at
                                the center of the bond. A molecular orbital whose sign is
                                unchanged by inversion is termed gerade, g, and one whose sign
                                is inverted is ungerade, u.
                                The total spin angular momentum quantum number, Σ, describes
                                the spin of the electrons in the molecule, and is quoted as its
                                multiplicity, (2Σ+1). The orbital angular momentum is described
                                by a quantum number A. For an electron in a a orbital, Λ=0, for
                                an electron in a π orbital, Λ=±1, etc. The term symbol
                                representing a specific electron configuration is written in the
                                                                          1
                                form  2Σ+1 Λ parity . The ground state of nitrogen is written as  Σ g , for
                                example.
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