Irreversible Processes and Entropy — Question 2

Section 20-1 · Physics pages 3234–3235

Question 2 Free expansion creates entropy even though no heat crosses the boundary One mole of ideal gas expands into vacuum inside a rigid insulated enclosure from volume V to 3V . Its internal energy depends only on temperature. To evaluate entropy, use any reversible reference path between the same equilibrium endpoints, with dS = δQrev/T and R = 8.314 J/(mol K). gas vacuum Schematic; labels, not drawing lengths, specify the data. (a) Find the actual heat, work and temperature change. (b) Use a reversible isothermal reference path to calculate entropy change. Identify the heat along that reference path at 300 K and explain why it is not the actual heat.
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Question 2 - Solution Free expansion creates entropy even though no heat crosses the boundary gas vacuum (a) Method and calculation Qactual = 0, Wactual = ∫ pextdV = 0, ∆U = 0 ⇒∆T = 0. pf/pi = Vi/Vf = 1/3. (b) Interpretation and further calculation ∆S = ∫3V V nRT dV/V T = nR ln 3 ≈9.13386 J/K. Qrev = nRT ln 3 ≈2740.16 J (T = 300 K). The reference path is a calculation device; entropy depends on endpoints, whereas heat depends on the actual process. Physical check Adiabatic does not mean isentropic when the process is irreversible.

Question 2

Free expansion creates entropy even though no heat crosses the boundary

One mole of ideal gas expands into vacuum inside a rigid insulated enclosure from volume VV to 3V3V. Its internal energy depends only on temperature. To evaluate entropy, use any reversible reference path between the same equilibrium endpoints, with dS=δQrev/TdS=\delta Q_{\mathrm{rev}}/T and R=8.314R=8.314 J/(mol K).

Diagram shown in the original SVG worksheet.

  1. Find the actual heat, work and temperature change.

  2. Use a reversible isothermal reference path to calculate entropy change. Identify the heat along that reference path at 300 K and explain why it is not the actual heat.

Question 2 - Solution

Free expansion creates entropy even though no heat crosses the boundary

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Qactual=0,Wactual=∫pextdV=0,ΔU=0⇒ΔT=0.Q_{\mathrm{actual}}=0,\quad W_{\mathrm{actual}}=\int p_{\mathrm{ext}}dV=0,\quad\Delta U=0\ \Rightarrow\Delta T=0.pf/pi=Vi/Vf=1/3.p_f/p_i=V_i/V_f=1/3.

(b) Interpretation and further calculation

ΔS=∫V3VnRTdV/VT=nRln⁡3≈9.13386J/K.\Delta S=\int_V^{3V}\frac{nRT\,dV/V}{T}=nR\ln3\approx9.13386\,\mathrm{J/K}.Qrev=nRTln⁡3≈2740.16J(T=300K).Q_{\mathrm{rev}}=nRT\ln3\approx2740.16\,\mathrm J\quad(T=300\,\mathrm K).The reference path is a calculation device; entropy depends on endpoints, whereas heat depends on the actual process.

Physical check

Adiabatic does not mean isentropic when the process is irreversible.