An Introduction to Thermal Physics · Problem 2.38

The Second Law — Daniel Schroeder

Physics — Statistical Mechanics · ideal-mixture-entropy

Problem

The mixing entropy formula derived in the previous problem actually applies to any ideal gas, and to some dense gases, liquids, and solids as well. For the denser systems, we have to assume that the two types of molecules are the same size and that molecules of different types interact with each other in the same way as molecules of the same type (same forces, etc.). Such a system is called an ideal mixture. Explain why, for an ideal mixture, the mixing entropy is given by ΔSmixing=kln⁡(NNA),\Delta S_{\text{mixing}} = k\ln\binom{N}{N_A}, where NN is the total number of molecules and NAN_A is the number of molecules of type AA. Use Stirling's approximation to show that this expression is the same as the result of the previous problem when both NN and NAN_A are large.

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