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H
θ
F
H
F
Figure 11.6 Experimentally observed structure for (HF) 2
interaction terms, going as R 4 , favour instead an L configuration
of the dimer, giving as a whole the structure of the homodimer with
u 60 observed by experiment and schematically represented in
Figure 11.6.
A similar result is obtained by the qualitative MO description of
the H-bond in (HF) 2 depicted in the drawings of Figure 11.7, which
showelectron transfer fromF lone pairs (doubly occupiedMOs) to a
vacant (empty MO) orbital on H. The top row shows
s
charge
transfer from F to H, the bottom row
charge transfer from F to H,
whichmust be doubled on account of the twofold degeneracy of the
p
p
p x MO). As a result, the dimer
roughly assumes the noncollinear geometrical structure 9 depicted in
Figure 11.6.
(b) As a further example, the leading R 6 term describing the polar-
ization of the He atom by the HF molecule, namely
energy level (the figure shows the
2
HF
3cos 2
ð 6 Þ¼ a
m
1
2
He
E ind
2
ð 11
:
56 Þ
R 6
.
H
F
H
F
H
.
F
H
F
Figure 11.7 MO description of the origin of the H-bond in (HF) 2
9 It must be remarked that molecular beam experimentalists refer to the geometrical shape of
Figure 11.6 as a linear dimer.
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