Some Special Cases of the First Law of Thermodynamics — Question 10

Section 18-10 · Physics pages 3010–3011

Question 10 A two-stage route separates isochoric and isothermal heating Use ∆U = Q −W, with work by the gas positive. The supplied gas model is pV = BT, with B = 10.0 J/K, and ∆U = CV ∆T, with total constant-volume heat capacity CV = 15.0 J/K. A gas starts at A with TA = 300 K and VA = .0100 m3. It first warms at fixed volume to B at 450 K, then expands quasistatically at 450 K to C with VC = .0200 m3. Only pressure-volume work occurs. V p Schematic equilibrium paths; process constraints determine the energy balance. (a) Find Q, W and ∆U for each stage and for the full route. (b) Compare with the reversed order: isothermal expansion at 300 K to .0200 m3, followed by fixed-volume warming to 450 K. Find the work and heat differences and explain why the final internal energy agrees.
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Question 10 - Solution A two-stage route separates isochoric and isothermal heating V p (a) Method and calculation WAB = 0, ∆UAB = QAB = 15(150) = 2250 J. ∆UBC = 0, WBC = QBC = 4500 ln 2 ≈3119.162 J. ∆UAC = 2250 J, WAC = 3119.162 J, QAC = 5369.162 J. (b) Interpretation and further calculation Wother = 3000 ln 2 ≈2079.442 J, Qother = 2250 + 2079.442 = 4329.442 J. ∆W = ∆Q = 1500 ln 2 ≈1039.721 J. The hotter isotherm gives more expansion work. Both routes end at the same T, V , so their common ∆U cancels when their first-law equations are subtracted. Physical check The additional heat for the first route equals its additional work because endpoint internal energy is unchanged between routes.

Question 10

A two-stage route separates isochoric and isothermal heating

Use ΔU=Q−W\Delta U=Q-W, with work by the gas positive. The supplied gas model is pV=BTpV=BT, with B=10.0J/KB=10.0\,\mathrm{J/K}, and ΔU=CVΔT\Delta U=C_V\Delta T, with total constant-volume heat capacity CV=15.0J/KC_V=15.0\,\mathrm{J/K}. A gas starts at A with TA=300T_A=300 K and VA=.0100m3V_A=.0100\,\mathrm{m^3}. It first warms at fixed volume to B at 450 K, then expands quasistatically at 450 K to C with VC=.0200m3V_C=.0200\,\mathrm{m^3}. Only pressure-volume work occurs.

Diagram shown in the original SVG worksheet.

  1. Find QQ, WW and ΔU\Delta U for each stage and for the full route.

  2. Compare with the reversed order: isothermal expansion at 300 K to .0200 m3^3, followed by fixed-volume warming to 450 K. Find the work and heat differences and explain why the final internal energy agrees.

Question 10 - Solution

A two-stage route separates isochoric and isothermal heating

Diagram shown in the original SVG worksheet.

(a) Method and calculation

WAB=0,ΔUAB=QAB=15(150)=2250J.W_{AB}=0,\quad\Delta U_{AB}=Q_{AB}=15(150)=2250\,\mathrm J.ΔUBC=0,WBC=QBC=4500ln⁡2≈3119.162J.\Delta U_{BC}=0,\quad W_{BC}=Q_{BC}=4500\ln2\approx3119.162\,\mathrm J.ΔUAC=2250J,WAC=3119.162J,QAC=5369.162J.\Delta U_{AC}=2250\,\mathrm J,\quad W_{AC}=3119.162\,\mathrm J,\quad Q_{AC}=5369.162\,\mathrm J.

(b) Interpretation and further calculation

Wother=3000ln⁡2≈2079.442J,Qother=2250+2079.442=4329.442J.W_{\mathrm{other}}=3000\ln2\approx2079.442\,\mathrm J,\quad Q_{\mathrm{other}}=2250+2079.442=4329.442\,\mathrm J.ΔW=ΔQ=1500ln⁡2≈1039.721J.\Delta W=\Delta Q=1500\ln2\approx1039.721\,\mathrm J.The hotter isotherm gives more expansion work. Both routes end at the same T,VT,V, so their common ΔU\Delta U cancels when their first-law equations are subtracted.

Physical check

The additional heat for the first route equals its additional work because endpoint internal energy is unchanged between routes.