Consider a cell with volume V , like those of Fig. 5.1, that has imaginary walls and

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Consider a cell with volume V , like those of Fig. 5.1, that has imaginary walls and is immersed in a bath of identical, nonrelativistic, classical perfect-gas particles with temperature Tb and chemical potential μb. Suppose that we make a large number of measurements of the number of particles in the cell and that from those measurements we compute the probability pN for that cell to contain N particles.


(a) How widely spaced in time must the measurements be to guarantee that the measured probability distribution is the same as that computed, using the methods of this section, from an ensemble of cells (Fig. 5.1) at a specific moment of time?


(b) Assume that the measurements are widely enough separated for this criterion to be satisfied. Show that pN is given by


image


where Ω(V, Tb, μb; N) is the grand potential for the ensemble of cells, with each cell constrained to have precisely N particles in it.(c) By evaluating Eq. (5.71) exactly and then computing the normalization constant, show that the probability pN for the cell to contain N particles is given by the Poisson distribution


image


where N̅ is the mean number of particles in a cell,


image


[Eq. (3.39a)].(d) Show that for the Poisson distribution (5.72a), the expectation value is (N) = N̅, and the rms deviation from this is


image


(e) Show that for image


this Poisson distribution is exceedingly well approximated by a Gaussian with mean N̅ and variance σN.



Eq. (3.39a)


image


Fig. 5.1


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