The Adiabatic Expansion of an Ideal Gas — Question 5

Section 19-10 · Physics pages 3220–3221

Question 5 An isothermal path and an adiabat from the same state do different work Use pV = nRT, R = 8.314 J/(mol K), and ∆U = Q −W with W positive for work done by the gas. One mole at 400 K expands reversibly to twice its initial volume. Compare an isothermal path with an adiabatic path having γ = 1.40 and CV = 5R/2. V p solid: isothermal dashed: adiabatic Axes and labels specify the model; the sketch is schematic. (a) Calculate work and heat for each path, including final adiabatic temperature. (b) Use the pressure curves to explain the work ordering. Do these paths reach the same final thermodynamic state?
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Question 5 - Solution An isothermal path and an adiabat from the same state do different work V p solid: isothermal dashed: adiabatic (a) Method and calculation WT = nRTi ln 2 ≈2305.130 J, ∆UT = 0 ⇒QT = WT . Tad,f = 400(2)−.400 ≈303.143 K. Qad = 0, Wad = 5 2R(400 −303.143) ≈2013.166 J. (b) Interpretation and further calculation For V > Vi, pT = pi(Vi/V ), pad = pi(Vi/V )γ < pT ⇒Wad < WT . Vf,T = Vf,ad = 2Vi, Tf,T̸ = Tf,ad. The final temperatures and pressures differ. Heat supplied along the isotherm maintains its higher pressure during expansion. Physical check The comparison holds fixed initial state and final volume, not fixed final temperature.

Question 5

An isothermal path and an adiabat from the same state do different work

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. One mole at 400 K expands reversibly to twice its initial volume. Compare an isothermal path with an adiabatic path having γ=1.40\gamma=1.40 and CV=5R/2C_V=5R/2.

Diagram shown in the original SVG worksheet.

  1. Calculate work and heat for each path, including final adiabatic temperature.

  2. Use the pressure curves to explain the work ordering. Do these paths reach the same final thermodynamic state?

Question 5 - Solution

An isothermal path and an adiabat from the same state do different work

Diagram shown in the original SVG worksheet.

(a) Method and calculation

WT=nRTiln⁡2≈2305.130J,ΔUT=0⇒QT=WT.W_T=nRT_i\ln2\approx2305.130\,\mathrm J,\quad\Delta U_T=0\ \Rightarrow\ Q_T=W_T.Tad,f=400(2)−.400≈303.143K.T_{{\mathrm{ad}},f}=400(2)^{-.400}\approx303.143\,\mathrm K.Qad=0,Wad=52R(400−303.143)≈2013.166J.Q_{\mathrm{ad}}=0,\quad W_{\mathrm{ad}}=\tfrac52R(400-303.143)\approx2013.166\,\mathrm J.

(b) Interpretation and further calculation

For V>ViV>V_i,pT=pi(Vi/V),pad=pi(Vi/V)γ<pT⇒Wad<WT.p_T=p_i(V_i/V),\quad p_{\mathrm{ad}}=p_i(V_i/V)^\gamma<p_T\ \Rightarrow\ W_{\mathrm{ad}}<W_T.Vf,T=Vf,ad=2Vi,Tf,T≠Tf,ad.V_{f,T}=V_{f,\mathrm{ad}}=2V_i,\quad T_{f,T}\ne T_{f,\mathrm{ad}}.The final temperatures and pressures differ. Heat supplied along the isotherm maintains its higher pressure during expansion.

Physical check

The comparison holds fixed initial state and final volume, not fixed final temperature.