The Adiabatic Expansion of an Ideal Gas — Question 10

Section 19-10 · Physics pages 3230–3231

Question 10 An adiabatic leg closes a three-process energy cycle Use pV = nRT, R = 8.314 J/(mol K), and ∆U = Q −W with W positive for work done by the gas. A .100 mol monatomic ideal gas starts at state A with temperature 600 K and volume V0. It expands reversibly and adiabatically to state B at 2V0, then is compressed at constant pB to state C at V0, then heated at fixed volume back to A. Use CV = 3R/2 and Cp = 5R/2. V p A B C Axes and labels specify the model; the sketch is schematic. (a) Find temperatures at B and C, and work for each leg. (b) Find heat for each leg and verify that total heat equals net work over the closed cycle. State the sign of net work.
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Question 10 - Solution An adiabatic leg closes a three-process energy cycle V p A B C (a) Method and calculation TB = 600(1/2)2/3 ≈377.976 K, TC = TB(VC/VB) ≈188.988 K. WAB = nCV (TA −TB) ≈276.886 J, WBC = nR(TC −TB) ≈−157.125 J. WCA = 0, Wnet ≈119.761 J. (b) Interpretation and further calculation QAB = 0, QBC = nCp(TC −TB) ≈−392.812 J. QCA = nCV (TA −TC) ≈512.573 J. Qnet = 512.573 −392.812 ≈119.761 J = Wnet, ∆Ucycle = 0. The clockwise cycle produces positive net work; heat entering on the isochore exceeds the heat rejected on the isobar. Physical check Work and heat depend on the route, but returning to the initial state forces the net internal-energy change to vanish.

Question 10

An adiabatic leg closes a three-process energy cycle

Use pV=nRTpV=nRT, R=8.314R=8.314 J/(mol K), and ΔU=Q−W\Delta U=Q-W with WW positive for work done by the gas. A .100 mol monatomic ideal gas starts at state A with temperature 600 K and volume V0V_0. It expands reversibly and adiabatically to state B at 2V02V_0, then is compressed at constant pBp_B to state C at V0V_0, then heated at fixed volume back to A. Use CV=3R/2C_V=3R/2 and Cp=5R/2C_p=5R/2.

Diagram shown in the original SVG worksheet.

  1. Find temperatures at B and C, and work for each leg.

  2. Find heat for each leg and verify that total heat equals net work over the closed cycle. State the sign of net work.

Question 10 - Solution

An adiabatic leg closes a three-process energy cycle

Diagram shown in the original SVG worksheet.

(a) Method and calculation

TB=600(1/2)2/3≈377.976K,TC=TB(VC/VB)≈188.988K.T_B=600(1/2)^{2/3}\approx377.976\,\mathrm K,\quad T_C=T_B(V_C/V_B)\approx188.988\,\mathrm K.WAB=nCV(TA−TB)≈276.886J,WBC=nR(TC−TB)≈−157.125J.W_{AB}=nC_V(T_A-T_B)\approx276.886\,\mathrm J,\quad W_{BC}=nR(T_C-T_B)\approx-157.125\,\mathrm J.WCA=0,Wnet≈119.761J.W_{CA}=0,\quad W_{\mathrm{net}}\approx119.761\,\mathrm J.

(b) Interpretation and further calculation

QAB=0,QBC=nCp(TC−TB)≈−392.812J.Q_{AB}=0,\quad Q_{BC}=nC_p(T_C-T_B)\approx-392.812\,\mathrm J.QCA=nCV(TA−TC)≈512.573J.Q_{CA}=nC_V(T_A-T_C)\approx512.573\,\mathrm J.Qnet=512.573−392.812≈119.761J=Wnet,ΔUcycle=0.Q_{\mathrm{net}}=512.573-392.812\approx119.761\,\mathrm J=W_{\mathrm{net}},\quad\Delta U_{\mathrm{cycle}}=0.The clockwise cycle produces positive net work; heat entering on the isochore exceeds the heat rejected on the isobar.

Physical check

Work and heat depend on the route, but returning to the initial state forces the net internal-energy change to vanish.