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Mg(OH) 2
Mg(OD) 2
0
500
1000
1500
2000
2500
3000
3500
4000
Wavenumber (cm -1 )
Figure 3.4
Energy shift in brucite (Mg(OH) 2 ) induced by the substitution of D for H in the OH radical (courtesy
of Bruno Reynard). Spectroscopists do not normally work with frequency but with wavenumbers,
in cm 1 , which are frequencies divided by the velocity of light.
Let us go back to the exchange of 16 O and 18 O between water vapor and liquid water
(3.1) and consider a vibrational mode with different hardness parameters k vap
k liq indica-
tive of loose bonds in the gaseous state ( Fig. 3.5 ) . The variation
E of energy during this
exchange is
E H 2 18 O vap +
E H 2 16 O liq
E H 2 18 O liq +
E H 2 16 O vap
E
=
(3.8)
or
E H 2 18 O vap
E H 2 16 O vap
E H 2 18 O liq
E H 2 16 O liq
E
=
(3.9)
For the sake of illustration, let us assume that most of the atoms will occupy their ground,
zero-point energy level ( n
=
0) so that:
2 h
ν H 2 18 O vap ν H 2 16 O vap
ν H 2 18 O liq ν H 2 16 O liq
1
E
=
(3.10)
k vap k liq
h
4
1
M H 1 2 O
1
M H 1 2 O
=
(3.11)
π
 
 
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