196 Problema E/ Solutio~ on Thermcdynamica d Statintical Mechanics
The specific heat at constant volume is
c, = (g) = Nok (2-)acsch2 (L)
V 2V kT 2VkT '
(b) As shown in Fig. 2.9.
Fig. 2.9.
(c) The equation of state is
p = - No - - a 1nz = - No'Y coth (&) ,
P av 2v2
where p is the pressure.
(d) The fraction of particles in the m-th level is
2034
The molecules of a certain gas consist of two different atoms, each with
zero nuclear spin, bound together. Measurements of the specific heat of this
material, over a wide range of temperatures, give the graph shown below.