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This is best discussed in the grand canonical ensemble (see Problem 8.4). From (8.48) all other thermodynamic functions can be determined after z is determined in terms of N from (8.46). The Boltzmann gas will be worked out explicitly. From (8.38) and (8.44) we have

(8.51)

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This quantity is called the thermal wavelength because it is of the order of the de Broglie wavelength of a particle of mass m with the energy kT. Writing v = V IN we obtain

DELETE: This call is similar to PUT, but allows the client to remove a file or Web page from the server It is also allowed to cause side effects in the same way as PUT Although available, the use of a DELETE call is not very common

(8.52)

Therefore T is the absolute temperature. The entropy is, by (8.48) and (8.46),

= 1N

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- N log -

Planck's constant follows from (8.31), where h first makes its appearance. The equation of state is deduced from the function U(S, V), which is E expressed in terms of S and V. We straightforwardly find PV = NkT. It is to be noted that (8.54) does not satisfy the third law of thermodynamics. This should cause no concern, because a Boltzmann gas is not a physical system. It is only a model toward which the Bose and Fermi gas converge at high temperatures. This shows, however, that the third law of thermodynamics is not an automatic consequence of the general principles of quantum mechanics, but depends on the nature of the density of states near the ground state. The Bose and Fermi gases can be worked out along similar lines. They are more conveniently discussed, however, in the grand canonical ensemble, which we consider in the next section.

QN(V, T) =

Given the simplicity of servlets, it makes sense to keep each servlet focused on a specific task, and then set u p multiple servlets to collaboratively achieve a more complex task Servlets can take care of the mechanical aspects of such collaborative efforts easily by implementing the RequestDispatcher interface

{ np}

(8.55)

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(8.56)

The RequestDispatcher interface provides two key capabilities:

(8.57)

For a Bose gas and a Boltzmann gas n p = 0,1,2, .... For a Fermi gas n p = 0,1. The number of states corresponding to {n p } is (Bose and Fermi) (Boltzmann)

(8.58)

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