PHYS6562 M5 Daily Question

Undistinguished particles and the Gibbs factor

(a) \[\Omega = \frac{V^N}{N!}\]

\[S = k_B \space \log(\Omega) = k_B(N\log(V) - B\log(N) + N) = Nk_B\left(1+\log\left(\frac{V}{N}\right) \right)\]

The average volume of a region for single particle is \(v = V/N\) with the entropy of \(s = k_B\log(v)\). Therefore, the configuration entropy is related to N times the entropy of a particle in its region with average volume.

(b) \[S = Nk_B\left(\frac{5}{2}-\log(\rho\lambda^3)\right) = Nk_B\left(\frac{5}{2}+\log\left(\frac{V}{N}\lambda^3\right)\right)\] The configuration entropy for an ideal gas particle is also related to the small average volume \(v\). \[S_c = Nk_B\log(v)\]

But the ideal gas particles also occupy the momentum space and each particle has the average length of \(\lambda\) in each dimension. So

\[S_p = 3Nk_B\log(\lambda) = Nk_B\log(\lambda^3)\]

Combine the configuration and momentum entropy for one particle, \[S = S_c+S_p = Nk_B\log(v*\lambda^3) = Nk_B\log\left(\frac{V}{N}*\lambda^3\right)\] The total entropy is related to the N times the space occupied both in configuration and momentum space.

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