A Statistical View of Entropy — Question 8

Section 20-7 · Physics pages 3366–3367

Question 8 Unequal state probabilities require a weighted entropy A system occupies four possible states with probabilities (1/2, 1/4, 1/4, 0). For this exercise use the ensemble entropy S = −kB ∑ i pi ln pi, with the continuous convention 0 ln 0 = 0. Compare with a uniform distribution over the same four states. state pi 1/2 1/4 1/4 0 1 2 3 4 Schematic; labels, not drawing lengths, specify the data. (a) Evaluate the entropy of the stated distribution and its deficit below the uniform value. (b) Explain why kB ln 3, obtained by counting nonzero-probability states, is incorrect here. Derive the reduction to kB ln Ωwhen all Ωprobabilities are equal.
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Question 8 - Solution Unequal state probabilities require a weighted entropy state pi 1/2 1/4 1/4 0 1 2 3 4 (a) Method and calculation S/kB = −1 2 ln 1 2 −2(1 4 ln 1 4) = 3 2 ln 2 ≈1.03972. Suniform/kB = ln 4 = 2 ln 2, (Suniform −S)/kB = 1 2 ln 2 ≈.346574. (b) Interpretation and further calculation pi = 1/Ω: S = −kBΩ(1/Ω) ln(1/Ω) = kB ln Ω. ln 3 ≈1.09861̸ = 3 2 ln 2. Counting occupied states alone would assign equal weight to three states, contradicting the specified probabilities. Physical check The zero-probability term vanishes by its limit; taking ln 0 alone would be an invalid intermediate step.

Question 8

Unequal state probabilities require a weighted entropy

A system occupies four possible states with probabilities (1/2,1/4,1/4,0)(1/2,1/4,1/4,0). For this exercise use the ensemble entropy S=−kB∑ipiln⁡piS=-k_B\sum_i p_i\ln p_i, with the continuous convention 0ln⁡0=00\ln0=0. Compare with a uniform distribution over the same four states.

Diagram shown in the original SVG worksheet.

  1. Evaluate the entropy of the stated distribution and its deficit below the uniform value.

  2. Explain why kBln⁡3k_B\ln3, obtained by counting nonzero-probability states, is incorrect here. Derive the reduction to kBln⁡Ωk_B\ln\Omega when all Ω\Omega probabilities are equal.

Question 8 - Solution

Unequal state probabilities require a weighted entropy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

S/kB=−12ln⁡12−2(14ln⁡14)=32ln⁡2≈1.03972.S/k_B=-\tfrac12\ln\tfrac12-2(\tfrac14\ln\tfrac14)=\tfrac32\ln2\approx1.03972.Suniform/kB=ln⁡4=2ln⁡2,(Suniform−S)/kB=12ln⁡2≈.346574.S_{\mathrm{uniform}}/k_B=\ln4=2\ln2,\quad(S_{\mathrm{uniform}}-S)/k_B=\tfrac12\ln2\approx.346574.

(b) Interpretation and further calculation

pi=1/Ω:S=−kBΩ(1/Ω)ln⁡(1/Ω)=kBln⁡Ω.p_i=1/\Omega:\quad S=-k_B\Omega(1/\Omega)\ln(1/\Omega)=k_B\ln\Omega.ln⁡3≈1.09861≠32ln⁡2.\ln3\approx1.09861\ne\tfrac32\ln2.Counting occupied states alone would assign equal weight to three states, contradicting the specified probabilities.

Physical check

The zero-probability term vanishes by its limit; taking ln⁡0\ln0 alone would be an invalid intermediate step.