386 Problems d Solutiom on Thermodynomic3 6' Statistical Mechanics
Thus the molecular flux along the pipe is
4 = -Avo An
Since
we have
1 kT
nu pa
1=-=-,
4 = Avo^1 dp
u pdz
(b) As given, p 5 lop5 rnmHg, we have
That is, the mean free path is much longer than the pipe and the above
expression for 4 is not valid. However, as the diameter of the pipe is much
smaller than its length, we have 4 = Avon.
Assume that both the initial and final states are in thermal equilibrium
at temperature T, then
dn
dt
V- =-A von ,
Hence
2194
Consider the hydrodynamical flow conditions. The cooling of the gas
during expansion can be expressed as follows, 5 = 1 + -, where To is
the temperature before expansion, T is the temperature after expansion,
M2
T 3