200 Problems €4 Sdutiom on Thermodylom'cs d Statiaticd Mechanics
(b) At high temperatures BIT << 1 and exp[-Oj(j + 1)/T) changes
slowly as j changes, so that we can think of (2j + 1) exp[-Oj(j + 1)/T] as
a continuous function of j. Let x = j(j + l), then dx = 2j + 1, and we can
write zo as an integral:(c) At high temperatures, the internal energy isa
aBU = --lnzo = IcT.
The heat capacity is
C,=k.(d) At low temperatures, we have T << 6, and exp[-6j(j + 1)/T] is
very small. We need only take the first two terms of zo, SO2037
The energy levels of a three-dimensional rigid rotor of moment of in-
ertial I are given by
EJ,M = h2J(J + 1)/2I ,
where J = 0,1,2,... ;M = -J, -J + 1,... , J. Consider a system of N
rotors:
(a) Using Boltzmann statistics, find an expression for the thermody-(b) Under what conditions can the sum in part (a) be approximatednamical internal energy of the system.by an integral? In this case calculate the specific heat C, of the system.
( wis co nsin)