Construct a partition function for the system

elduderino
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Homework Statement



Consider a system of N noninteracting particles in a container of cross-sectional area A. Bottom of the container is rigid. The top consists of an airtight, frictionless piston of mass M. Neglect the potential energy of the molecules of gas.

Construct the partition function Q of the (N+1) particle system (N particles of mass m+ piston)

Calculate the fluctuations in the volume of the system?

Homework Equations


Z= \frac{1}{N!h^{3N}}\int e^{-\beta H(p,q)}d^3pd^3q

The Attempt at a Solution



System is in equilibrium for theory to be applicable, hence piston is at rest at some height y.

H(p,q) = \sum_i \frac{p_i^2}{2m} +mgy

6N+1 dimensional phase space

Z= \frac{1}{N!h^{3N}}\int e^{-\beta (\sum_i \frac{p_i^2}{2m} +mgy )}d^3pd^3q dy
 
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Addition: I did the integration for Z but the answer is not coming right. How do I know the answer? It SHOULD come out to be the same as the Gibb's potential for an ideal gas. ie A=-kTlnZ.
 
To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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