2 In the solid of Einstein, we may introduce a volume coordinate if we make the phenomenological assumption that the fundamental fre- V/N is given by quency w as a function of v = (:) w =w (v) = wo – A ln where wo, A, and v, are positive constants. Obtain expressions for the expansion coefficient and the isothermal compressibility of this model system.
2 In the solid of Einstein, we may introduce a volume coordinate if we make the phenomenological assumption that the fundamental fre- V/N is given by quency w as a function of v = (:) w =w (v) = wo – A ln where wo, A, and v, are positive constants. Obtain expressions for the expansion coefficient and the isothermal compressibility of this model system.
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Statistical Physics. Microcanonical Ensemble.

Transcribed Image Text:4.2 In the solid of Einstein, we may introduce a volume coordinate if
we make the phenomenological assumption that the fundamental fre-
quency w as a function of v = V/N is given by
w =w (v) = w. – A ln
Vo
where wo, A, and v, are positive constants. Obtain expressions for
the expansion coefficient and the isothermal compressibility of this
model system.
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