Find thermodynamic generalized force

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SUMMARY

The discussion focuses on calculating the work done on a microscopic pendulum modeled as a quantum harmonic oscillator and determining the thermodynamic generalized force. The partition function is derived as ##Z= \frac{1}{2\sinh(\beta\hbar\omega/2)}##, where ##\epsilon_n = \hbar\omega(1/2 + n)## and ##\beta= \frac{1}{kT}##. The Helmholtz Free Energy is expressed as ##F = U - TS = -kT\ln{Z}##, leading to the relationship ##U = F - T\frac{\partial F}{\partial T}##. The challenge lies in computing the thermodynamic generalized force ##F_x## due to the dependency of ##\omega## on the pendulum length ##l##.

PREREQUISITES
  • Understanding of quantum harmonic oscillators
  • Familiarity with partition functions in statistical mechanics
  • Knowledge of Helmholtz Free Energy and its derivation
  • Basic concepts of thermodynamic generalized forces
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  • Study the relationship between pendulum length variations and frequency changes
  • Explore the derivation of thermodynamic generalized forces in quantum systems
  • Learn about the implications of the partition function on thermodynamic properties
  • Investigate the role of temperature in the behavior of quantum harmonic oscillators
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Physicists, particularly those specializing in statistical mechanics and thermodynamics, as well as students and researchers interested in quantum systems and their thermodynamic properties.

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Homework Statement
Statistical Mechanics
Relevant Equations
Canonical Ensemble, Thermodynamic generalized forces
Assume you have a microscopic pendulum you can suppose is like quantum harmonic oscillator. If the length of pendulum has variation of ##dl##, calculate the work on the pendulum and thermodynamic generalized force.
Find also the variation of mean number of extitations.


My Attempt

Firstly, I find the partition function: ##Z= \sum_n e^{-\beta\epsilon_n}##, with ##\epsilon_n = \hbar\omega(1/2 + n)## and this is the result:

##Z= \frac{1}{2sinh(\beta\hbar\omega/2)}##.

In this result ##\beta= \frac{1}{kT}##.

Then, I can write Helmholtz Free Energy: ##F = U -TS = -kT\ln{Z}##

And of course ## U = F-T\frac{\partial F}{\partial T}##


I know that ##-\frac{\partial U}{\partial x} = F_x## but if i don't know how thermodynamic variables depends on ##l## how I can compute the thermodynamic generalized force?
 
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##\omega## depends on l.
 
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