A Statistical View of Entropy — Question 7

Section 20-7 · Physics pages 3364–3365

Question 7 Binary composition entropy has a calculable maximum A large collection has N distinguishable sites, with Nx occupied by species A and N(1 −x) by B. For fixed counts, Ω= N!/[(Nx)!(N(1 −x))!]. Use the leading Stirling approximation ln m! ≃m ln m −m, with both species counts large. x h(x) 1/2 1 Axes and labels specify the model; the sketch is schematic. (a) Derive the leading configurational entropy per site and evaluate it at x = .200 and x = .500. (b) Differentiate to locate and classify the maximum. Explain why changing the species fraction changes the number of arrangements at fixed N.
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Question 7 - Solution Binary composition entropy has a calculable maximum x h(x) 1/2 1 (a) Method and calculation S kB = ln N! −ln(Nx)! −ln[N(1 −x)]!. S NkB ≃−x ln x −(1 −x) ln(1 −x) ≡h(x). h(.200) ≈.500402, h(.500) = ln 2 ≈.693147. (b) Interpretation and further calculation h′(x) = ln 1 −x x = 0 ⇒x = 1/2. h′′(x) = −1/x −1/(1 −x) < 0. At equal composition there are the most ways to assign the two species to sites. This is a configurational count; any energy differences would require additional statistical weights. Physical check The approximation neglects subleading terms in ln N; it is not an exact finite-N entropy formula.

Question 7

Binary composition entropy has a calculable maximum

A large collection has NN distinguishable sites, with NxNx occupied by species A and N(1−x)N(1-x) by B. For fixed counts, Ω=N!/[(Nx)!(N(1−x))!]\Omega=N!/[(Nx)!(N(1-x))!]. Use the leading Stirling approximation ln⁡m!≃mln⁡m−m\ln m!\simeq m\ln m-m, with both species counts large.

Diagram shown in the original SVG worksheet.

  1. Derive the leading configurational entropy per site and evaluate it at x=.200x=.200 and x=.500x=.500.

  2. Differentiate to locate and classify the maximum. Explain why changing the species fraction changes the number of arrangements at fixed NN.

Question 7 - Solution

Binary composition entropy has a calculable maximum

Diagram shown in the original SVG worksheet.

(a) Method and calculation

SkB=ln⁡N!−ln⁡(Nx)!−ln⁡[N(1−x)]!.\frac{S}{k_B}=\ln N!-\ln(Nx)!-\ln[N(1-x)]!.SNkB≃−xln⁡x−(1−x)ln⁡(1−x)≡h(x).\frac{S}{Nk_B}\simeq-x\ln x-(1-x)\ln(1-x)\equiv h(x).h(.200)≈.500402,h(.500)=ln⁡2≈.693147.h(.200)\approx.500402,\quad h(.500)=\ln2\approx.693147.

(b) Interpretation and further calculation

h′(x)=ln⁡1−xx=0⇒x=1/2.h\prime(x)=\ln\frac{1-x}{x}=0\Rightarrow x=1/2.h′′(x)=−1/x−1/(1−x)<0.h\prime\prime(x)=-1/x-1/(1-x)<0.At equal composition there are the most ways to assign the two species to sites. This is a configurational count; any energy differences would require additional statistical weights.

Physical check

The approximation neglects subleading terms in ln⁡N\ln N; it is not an exact finite-NN entropy formula.