27.4 Classical Statistical Mechanics 1137
The result of this example is
zrot,cl 8 π^2 IekBT
(
diatomic or linear polyatomic substance
)
(27.4-14)
whereIeis the moment of inertia of the molecule. The derivation of the rotational
factor in the classical partition function for a nonlinear polyatomic substance is even
more complicated, and we simply present the result:
zrot,cl
√
π(8π^2 kBT)^3 /^2 (IAIBIC)^1 /^2
(
nonlinear polyatomic substance
)
(27.4-15)
whereIA,IB, andICare the principal moments of inertia as defined in Chapter 22.
We represent the vibration of a diatomic molecule by a harmonic oscillator with
massμ(the reduced mass of the molecule) and frequencyν. The classical vibrational
partition function for a harmonic oscillator is
zvib,cl
∫∞
−∞
exp
[
−
p^2 / 2 μ
kBT
]
dp
∫∞
−∞
exp
[
−
kx^2 / 2
kBT
]
dx
(2πμkBT)^1 /^2 (2πkBT/k)^1 /^2
(2πkBT)
√
μ
k
kBT
ν
(dilute diatomic gas) (27.4-16)
whereμis the reduced mass,kis the force constant, andνis the frequency of the
oscillator, from Eq. (14.2-24). We have used infinite limits for the integrations since
the harmonic oscillator is not limited to a finite range of oscillation. For a polyatomic
substance, there is one factor like that of Eq. (27.4-16) for each normal mode:
zvib,cl
3 n∏−5(6)
i 1
kBT
νi
(dilute polyatomic gas) (27.4-17)
where the limit on the product indicates 3n−5 normal modes for a linear molecule
and 3n−6 normal modes for a nonlinear molecule. We will not attempt to discuss
electronic motion classically, but assume that electronic excitation can be ignored.
For diatomic and polyatomic dilute gases without electronic excitation we have the
same relation as for monatomic gases:
ZclzNcl (27.4-18)
where
zclztr,clzrot,clzvib,cl
(
any dilute gas without eletronic excitation
)
(27.4-19)
Comparison of the Classical and Quantum Partition
Functions
The translational factor of the classical molecular partition function is proportional to
the quantum mechanical translational factor:
ztr,qm
(
2 πmkBT
h^2
) 3 / 2
V
ztr,cl
h^3