c18 JWBS043-Rogers September 13, 2010 11:29 Printer Name: Yet to Come
DIPOLE MOMENTS 295
Thedielectric constantof substancexis defined as the ratio
εx=
Cx
C 0
which is always greater than one. Dielectric constants are very different for different
molecules; for example, the dielectric constants are 1.000272 for H 2 (g), 2.283 for
benzene, and 78.0 for water at 298 K. We describe benzene as anonpolarsolvent
and we describe water as apolarsolvent.
The molar polarization of a substancePis related to the dielectric constant by
P=
ε− 1
ε+ 2
M
ρ
where M is the molar mass. This is sometimes called thetotal molar polarization
because it is made up of two parts: thedistortion polarizationand theorientation
polarization,PT=Pd+Po.
Distortion polarization exists for all substances, which is the reason thatεis never
less than one. Consider a collection of atoms of a monatomic gas such as neon or
argon. The electronic charge distribution within each atom is spherically symmetrical
in the absence of a field; but in the presence of a field, the atomic charge distribution
is distorted into something like the ellipses shown in Fig. 18.7, and a dipolar nature
isinducedin it.
Orientation polarization results from the permanent dipole brought about by an
unsymmetrical charge distribution in the unperturbed molecule. A familiar example
is HCl, which has a negative end (Cl) and a positive end (H).
The mathematical form of these two distinct types of polarization enables us to
determine both. Distortion polarization is not a function of temperature,
Pd=
4
3
πNAα
but orientation polarization is inversely dependent uponT:
Po=
4 πNA
9 kBT
μ^2
whereNAis the Avogadro number andkB is the Boltzmann constant. One can
rearrange the equation for the total polarization as a function of 1/Tto emphasize its
linear nature:
PT=
4 πNAμ^2
9 kB
1
T
+
4
3
πNAα=
4 πNA
3
[(
μ^2
3 kB
)
1
T
+α