Find thermodynamic generalized force

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The discussion focuses on calculating the work done on a microscopic pendulum modeled as a quantum harmonic oscillator, specifically when the pendulum's length varies by ##dl##. The partition function is derived as ##Z= \frac{1}{2sinh(\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 internal energy relation ##U = F - T\frac{\partial F}{\partial T}##. A challenge arises in determining the thermodynamic generalized force since the dependence of thermodynamic variables on the length ##l## is unclear, particularly how ##\omega## varies with ##l##. The discussion highlights the complexity of linking microscopic properties to macroscopic thermodynamic forces.
damarkk
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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.
 
At first, I derived that: $$\nabla \frac 1{\mu}=-\frac 1{{\mu}^3}\left((1-\beta^2)+\frac{\dot{\vec\beta}\cdot\vec R}c\right)\vec R$$ (dot means differentiation with respect to ##t'##). I assume this result is true because it gives valid result for magnetic field. To find electric field one should also derive partial derivative of ##\vec A## with respect to ##t##. I've used chain rule, substituted ##\vec A## and used derivative of product formula. $$\frac {\partial \vec A}{\partial t}=\frac...