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graphic, as the spheres used to mark the H atom positions are largely outside of the orbital
contour. The next level, 1 b 2 , does contribute to bonding, being formed from the 2p y and
the b 2 H(1s) SALC, which are much closer to one another. Similarly, the 3 a 1 level contains
significant contributions from both the O(2p z ) orbital and H(1s) a 1 SALC.
The HOMO is the nonbonding 1 b 1 level. This is the O(2p x ) AO, which is perpendicu-
lar to the plane of the molecule. The unoccupied orbitals are the antibonding 4 a 1 and 2 b 2
levels.
The weak involvement of the H(1s) orbitals in the 2 a 1 state leads to a bond order
estimate of 2 split evenly over the two O H bonds so that each is a single bond.
Water is an essential component of biological systems and has many interesting phys-
ical properties. For example, the density of ice at 0 C is actually less than that of the
liquid state, and so the solid floats. This is unusual, since for most other molecules
the intermolecular forces cause a denser packing in the solid state. However, the
intermolecular bonding for H 2 O is directional in nature due to hydrogen bonding. The
electronegativity of O is higher than H, and so the OH bonds are polarized to give posi-
tively charged H atoms and a negatively charged O. In addition, the nonbonding electrons
on O lead to an anisotropic distribution of electron density at O, commonly referred to as
the O lone pairs. To obtain optimal intermolecular H bonding the structure that ice adopts
is quite open, leading to a low density compared with the liquid state.
Problem 7.10: In Figure 7.25 we compare the energy levels for NH 3 in C 3v and D 3h
geometries. Here, H 2 O is taken to be C 2v , whereas we have seen that BeH 2 is a linear
D h molecule with the MO diagram given in Figure 7.16. Draw a diagram linking the
O atomic states in the alternative geometries and so demonstrate that the H 2 O structure
is preferred when the 3 a 1 state is occupied.
7.5 The Second-Row Diatomic Molecules
7.5.1 Homonuclear Diatomics
All the molecules considered so far have had H as one of the participants in the bonding
scheme. In this section we will start to consider the MOs produced for interactions between
heavier atoms, beginning with homonuclear diatomics, A 2 , of second-row elements. Gen-
eral MO diagrams for these diatomics will be constructed and then used to discuss the
relative stability of those that are observed experimentally: N 2 ,O 2 and F 2 and those that
are not found under normal circumstances, Li 2 ,Be 2 ,B 2 and C 2 . In common with H 2 , these
molecules all belong to the D h point group and so the 2s valence orbitals will be linked
together as
σ g + and
σ u + SALCs:
1
2 ( s 1 +
σ g + =
s 2 )
(7.60)
1
2
σ u + =
( s 1
s 2 )
(7.61)
 
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