The Adiabatic Expansion of an Ideal Gas — Question 7

Section 19-10 · Physics pages 3224–3225

Question 7 Expansion against a fixed load requires external-pressure 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 of monatomic ideal gas starts at (pi, Vi, 500 K). A latched insulating piston is released against a constant external pressure pe = pi/2. It settles at pf = pe with zero final piston kinetic energy. Any transient mechanical energy is dissipated inside the gas; the piston and walls retain no energy. The gas is insulated. gas pe = pi/2 Schematic; labels, not drawing lengths, specify the data. (a) Find Tf, Vf/Vi and work done by the gas using W = pe(Vf −Vi). (b) Compare with reversible adiabatic expansion to the same final pressure and test whether the actual endpoints obey pV 5/3 = constant.
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Question 7 - Solution Expansion against a fixed load requires external-pressure work gas pe = pi/2 (a) Method and calculation nCV (Tf −Ti) = −pe(Vf −Vi), peVf = nRTf, peVi = 1 2nRTi. (CV + R)Tf = (CV + 1 2R)Ti ⇒Tf = 4 5Ti = 400 K. Vf/Vi = (Tf/Ti)/(pf/pi) = 1.60, W = 3 2R(100) = 1247.10 J. (b) Interpretation and further calculation Tf,rev = 500(pf/pi)(γ−1)/γ = 500(1/2)2/5 ≈378.929 K. Wrev ≈1509.875 J, pfV 5/3 f piV 5/3 i = 1 2(1.60)5/3 ≈1.09438̸ = 1. Finite mechanical imbalance makes the actual path irreversible, despite zero heat transfer. Physical check The reversible and fixed-load paths have the same final pressure but different final temperatures and volumes.

Question 7

Expansion against a fixed load requires external-pressure 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 of monatomic ideal gas starts at (pi,Vi,500K)(p_i,V_i,500\,\mathrm K). A latched insulating piston is released against a constant external pressure pe=pi/2p_e=p_i/2. It settles at pf=pep_f=p_e with zero final piston kinetic energy. Any transient mechanical energy is dissipated inside the gas; the piston and walls retain no energy. The gas is insulated.

Diagram shown in the original SVG worksheet.

  1. Find TfT_f, Vf/ViV_f/V_i and work done by the gas using W=pe(Vf−Vi)W=p_e(V_f-V_i).

  2. Compare with reversible adiabatic expansion to the same final pressure and test whether the actual endpoints obey pV5/3=constantpV^{5/3}=\text{constant}.

Question 7 - Solution

Expansion against a fixed load requires external-pressure work

Diagram shown in the original SVG worksheet.

(a) Method and calculation

nCV(Tf−Ti)=−pe(Vf−Vi),peVf=nRTf,peVi=12nRTi.nC_V(T_f-T_i)=-p_e(V_f-V_i),\quad p_eV_f=nRT_f,\quad p_eV_i=\tfrac12nRT_i.(CV+R)Tf=(CV+12R)Ti⇒Tf=45Ti=400K.(C_V+R)T_f=(C_V+\tfrac12R)T_i\ \Rightarrow\ T_f=\tfrac45T_i=400\,\mathrm K.Vf/Vi=(Tf/Ti)/(pf/pi)=1.60,W=32R(100)=1247.10J.V_f/V_i=(T_f/T_i)/(p_f/p_i)=1.60,\quad W=\tfrac32R(100)=1247.10\,\mathrm J.

(b) Interpretation and further calculation

Tf,rev=500(pf/pi)(γ−1)/γ=500(1/2)2/5≈378.929K.T_{f,\mathrm{rev}}=500(p_f/p_i)^{(\gamma-1)/\gamma}=500(1/2)^{2/5}\approx378.929\,\mathrm K.Wrev≈1509.875J,pfVf5/3piVi5/3=12(1.60)5/3≈1.09438≠1.W_{\mathrm{rev}}\approx1509.875\,\mathrm J,\quad\frac{p_fV_f^{5/3}}{p_iV_i^{5/3}}=\tfrac12(1.60)^{5/3}\approx1.09438\ne1.Finite mechanical imbalance makes the actual path irreversible, despite zero heat transfer.

Physical check

The reversible and fixed-load paths have the same final pressure but different final temperatures and volumes.