More Graduate
Statistical Mechanics Problems, Fall 2004
- Calculate the partition function for a 2-D ideal Bose
gas in the thermodynamic limit (area taken to infinity). Find the average
number of particles per unit area as a function of the chemical potential
and temperature. Prove that in 2-D the specific heat of an ideal gas of
fermions is the same as for bosons for all values of N and T.
- The van der Waals equation
exhibits a critical point when both the 1st and 2nd
derivatives of the pressure with respect to volume at fixed T vanish. From
this condition, find Pc, Tc and Vc in terms of
parameters a,b. Show
that the equation of state can be written in an universal form in terms of
Pc, Vc and Tc. Sketch the P-V phase diagram for
various temperatures above, below and at Tc. Identify the sign of the
isothermal compressibility in each region and identify any unphysical
regions.
- Calculate the ratio of the isothermal compressibility
for a van der Waals gas and an ideal gas. Sketch
its behavior for various values of T as a function of volume V. Identify
all unphysical regions.
- Mechanical
model of a phase transition: Consider a mass m suspended between
points P1 and P2 by two identical springs with spring constant k and
equilibrium length l0. Let the points P1 and P2 be separated by
2L. Assume Hooke’s law to hold and that the mass
is always close to a symmetry point P0 that it is sufficient to expand the
potential up to 4th order in the distance of m from P0.
- Show that
for L>l0 , P0 is the
equilibrium point while for L<l0 every point on a circle
with radius r0 around P0 is an equilibrium position. Calculate and draw
r0 as a function of L.
- Calculate
and discuss the eigenfrequencies and eigenvectors for small oscillations
around the equilibrium positions as a function of L. Draw all eigenfrequencies as a function of L.
- Same as (b) but now assume a
constant force F acts in the same plane as the circle of equilibrium
positions. Consider r0 and the eigenfrequencies
now as functions of L and F.