6 Problems on Statistical Physics - Problem Set 4 | PHY 831, Assignments of Statistical mechanics

Material Type: Assignment; Class: Statistical Mechanics; Subject: Physics; University: Michigan State University; Term: Fall 2002;

Typology: Assignments

Pre 2010

Uploaded on 07/23/2009

koofers-user-g82-3
koofers-user-g82-3 🇺🇸

5

(1)

10 documents

1 / 1

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
Physics 831 - 2002
Statistical Physics
Problem Set 4
1. Calculate the constant
Cn=ZPx2
i<1
n
Y
i=1
dxi
using mathematical induction and the fact that C2=πand C3= 4π/3. Compare with the
result in the textbook [in particular, calculate Γ(2) and Γ(5/2)]. (5 pt)
2. Problem 6.4 [for the case of different gases] (3 pt)
3. Problem 6.3 (a) - (c) (6 pt)
4. Consider equilibrium of a body in an external time-independent field, for example, in grav-
itational field. The system is no longer spatially uniform. Still equilibrium with respect to
particle exchange requires that µ= const, but now the chemical potential may depend on
coordinates. In a gravitational field, the energy of a particle of a mass mhas just an extra
term u(r) = mgz. Then the chemical potential per particle has the form
µ(P, T ) = µ0(P, T ) + u(r),
where µ0is the chemical potential in the absence of the field. Prove this relation (3 pt) and
derive the equation for Pas a function of coordinates for a compressible system (3 pt).
5. Problem 6.1 (4 pt)
6. Problem 6.2 (4 pt)
The problems are from Kerson Huang, Statistical Mechanics, 2nd edition, (Wiley, NY 1987).

Partial preview of the text

Download 6 Problems on Statistical Physics - Problem Set 4 | PHY 831 and more Assignments Statistical mechanics in PDF only on Docsity!

Physics 831 - 2002

Statistical Physics

Problem Set 4

  1. Calculate the constant Cn =

∫ ∑ (^) x 2 i <^1

∏^ n i=

dxi

using mathematical induction and the fact that C 2 = π and C 3 = 4π/3. Compare with the result in the textbook [in particular, calculate Γ(2) and Γ(5/2)]. (5 pt)

  1. Problem 6.4 [for the case of different gases] (3 pt)
  2. Problem 6.3 (a) - (c) (6 pt)
  3. Consider equilibrium of a body in an external time-independent field, for example, in grav- itational field. The system is no longer spatially uniform. Still equilibrium with respect to particle exchange requires that μ = const, but now the chemical potential may depend on coordinates. In a gravitational field, the energy of a particle of a mass m has just an extra term u(r) = mgz. Then the chemical potential per particle has the form

μ(P, T ) = μ 0 (P, T ) + u(r),

where μ 0 is the chemical potential in the absence of the field. Prove this relation (3 pt) and derive the equation for P as a function of coordinates for a compressible system (3 pt).

  1. Problem 6.1 (4 pt)
  2. Problem 6.2 (4 pt)

The problems are from Kerson Huang, Statistical Mechanics, 2nd edition, (Wiley, NY 1987).