Blundell Thermal Physics · Problem 22.2

The chemical potential

Physics — Statistical Mechanics · fugacity-ideal-gas

Problem

The fugacity zz is defined as z=eβμz = e^{\beta\mu}. Using eqn 22.15, show that z=nλth3(22.102)z = n\lambda^3_\mathrm{th} \tag{22.102} for an ideal gas, and comment on the limits z≪1z \ll 1 and z≫1z \gg 1.

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