Change in Entropy — Question 8

Section 20-2 · Physics pages 3266–3267

Question 8 A nonuniform temperature field has an entropy below its uniform equilibrium A thin insulated rod has uniform heat capacity per length C/L, with total C = 100 J/K. Initially T(x) = 300 + 300x/L K for 0 ≤x ≤L. Ignore expansion, work and temperature dependence of capacity. Internal conduction brings it to uniform temperature. x T solid: initial; dashed: final Axes and labels specify the model; the sketch is schematic. (a) Find final temperature and express entropy change as a spatial integral. (b) Evaluate the integral using ∫ln T dT = T ln T −T. Explain why replacing the initial field by its mean would miss entropy generation.
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Question 8 - Solution A nonuniform temperature field has an entropy below its uniform equilibrium x T solid: initial; dashed: final (a) Method and calculation Tf = 1 L ∫L 0 T(x)dx = 450 K. ∆S = C L ∫L 0 ln 450 T(x)dx = C 300 ∫600 300 ln 450 T dT. (b) Interpretation and further calculation ∆S = C [1 + ln(450/300) −2 ln 2] ≈1.91707 J/K. Sgen = ∆S > 0. Averaging temperature preserves energy for constant capacity, but entropy depends on the spatial average of the logarithm, not the logarithm of the average. Physical check The logarithm is concave, so a uniform field maximizes entropy at fixed total thermal energy.

Question 8

A nonuniform temperature field has an entropy below its uniform equilibrium

A thin insulated rod has uniform heat capacity per length C/LC/L, with total C=100C=100 J/K. Initially T(x)=300+300x/LT(x)=300+300x/L K for 0≤x≤L0\le x\le L. Ignore expansion, work and temperature dependence of capacity. Internal conduction brings it to uniform temperature.

Diagram shown in the original SVG worksheet.

  1. Find final temperature and express entropy change as a spatial integral.

  2. Evaluate the integral using ∫ln⁡TdT=Tln⁡T−T\int\ln T\,dT=T\ln T-T. Explain why replacing the initial field by its mean would miss entropy generation.

Question 8 - Solution

A nonuniform temperature field has an entropy below its uniform equilibrium

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Tf=1L∫0LT(x)dx=450K.T_f=\frac1L\int_0^LT(x)dx=450\,\mathrm K.ΔS=CL∫0Lln⁡450T(x)dx=C300∫300600ln⁡450TdT.\Delta S=\frac CL\int_0^L\ln\frac{450}{T(x)}dx=\frac C{300}\int_{300}^{600}\ln\frac{450}{T}\,dT.

(b) Interpretation and further calculation

ΔS=C[1+ln(450/300)−2ln2]≈1.91707J/K.\Delta S=C\left[1+\ln(450/300)-2\ln2\right]\approx1.91707\,\mathrm{J/K}.Sgen=ΔS>0.S_{\mathrm{gen}}=\Delta S>0.Averaging temperature preserves energy for constant capacity, but entropy depends on the spatial average of the logarithm, not the logarithm of the average.

Physical check

The logarithm is concave, so a uniform field maximizes entropy at fixed total thermal energy.