Linear degree of freedom - Equipartition theorem

Click For Summary
SUMMARY

The discussion focuses on deriving the equipartition theorem for a linear degree of freedom characterized by the energy equation E = c|q|. The key equations involved include the partition function Z = ∑ e^{-\beta E(q)} and Z = (1/Δq) ∫_{-\infty}^{+\infty} e^{-\beta c |q|}dq. The integral must be evaluated from 0 to ∞ rather than from -∞ to ∞ to yield a meaningful result, leading to the conclusion that the average energy equals kT.

PREREQUISITES
  • Understanding of classical mechanics and degrees of freedom
  • Familiarity with the equipartition theorem
  • Knowledge of partition functions in statistical mechanics
  • Ability to perform integrals involving exponential functions
NEXT STEPS
  • Study the derivation of the equipartition theorem for quadratic degrees of freedom
  • Learn about the implications of linear versus quadratic energy functions in statistical mechanics
  • Explore advanced techniques for evaluating improper integrals
  • Investigate the role of the partition function in thermodynamic systems
USEFUL FOR

Students of physics, particularly those studying statistical mechanics, as well as educators and researchers looking to deepen their understanding of the equipartition theorem and its applications in classical systems.

steve233
Messages
17
Reaction score
0

Homework Statement



Consider a classical 'degree of freedom' that is linear rather than quadratic: E = c|q| for some constant c. Derive the equipartition theorem using this energy and show that the average energy is Ebar = kT.


Homework Equations



Z = \sum e^{-\beta E(q)} = \sum e^{-\beta c|q|}

Z = \frac{1}{\Delta q} \int_{-\infty}^{+\infty} e^{-\beta c |q|}dq

The Attempt at a Solution


The question seems straight forward, but I'm having a hard time grasping it.

Using the second equation, If I carry out that integral I get:

\frac{1}{\Delta q} \frac {-1}{\beta c} \left [ e^{-\beta cq} \right ]_{-\infty}^{+\infty} = 0

Which doesn't help at all. I'm not sure if there is a trick to the integral or I have to use another method.

Any help will be much appreciated.

PS. This is coursework but not a homework question. I am just doing this question to study for a test.
 
Physics news on Phys.org
it works if you go from zero to infinity on the bounds. and not -inf to +inf.
then use the formula <E>=-1/Z(dz/dB)
 

Similar threads

Replies
1
Views
2K
Replies
2
Views
2K
Replies
19
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
2
Views
4K
Replies
4
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K