A Closer Look at Heat and Work — Question 3

Section 18-8 · Physics pages 2956–2957

Question 3 External pressure determines work in an irreversible expansion A gas initially occupies 2.00 L at 400 kPa. It expands against a constant external pressure of 100 kPa until its volume is 6.00 L. The intermediate gas pressure is not uniform. For boundary work use W = ∫pext dV . V p pext Schematic pressure–volume paths; work is the signed area under a process curve. (a) Find work done by the gas. Assess the calculation pi(Vf −Vi). (b) Compare with a separate quasistatic route having p(V ) = 800/V kPa when V is numerically in litres, over the same volume interval. Must its final pressure equal the irreversible run's final pressure?
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Question 3 - Solution External pressure determines work in an irreversible expansion V p pext (a) Method and calculation Wirr = 100(6 −2) = 400 J. pi∆V = 400(4) = 1600 J̸ = Wirr. The initial internal pressure is not the resisting pressure throughout the displacement. (b) Interpretation and further calculation Wqs = ∫6 2 800 V dV J = 800 ln 3 J ≈878.890 J. pf,qs = 800/6 = 133.333 kPa. The endpoints share volumes but need not share final thermodynamic states; the irreversible run can finish at 100 kPa if mechanical equilibrium is reached. Physical check An equilibrium pV curve is not automatically available during a strongly irreversible process.

Question 3

External pressure determines work in an irreversible expansion

A gas initially occupies 2.00 L at 400 kPa. It expands against a constant external pressure of 100 kPa until its volume is 6.00 L. The intermediate gas pressure is not uniform. For boundary work use W=∫pextdVW=\int p_{\mathrm{ext}}\,dV.

Diagram shown in the original SVG worksheet.

  1. Find work done by the gas. Assess the calculation pi(Vf−Vi)p_i(V_f-V_i).

  2. Compare with a separate quasistatic route having p(V)=800/Vp(V)=800/V kPa when VV is numerically in litres, over the same volume interval. Must its final pressure equal the irreversible run's final pressure?

Question 3 - Solution

External pressure determines work in an irreversible expansion

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Wirr=100(6−2)=400J.W_{\mathrm{irr}}=100(6-2)=400\,\mathrm J.piΔV=400(4)=1600J≠Wirr.p_i\Delta V=400(4)=1600\,\mathrm J\ne W_{\mathrm{irr}}.The initial internal pressure is not the resisting pressure throughout the displacement.

(b) Interpretation and further calculation

Wqs=∫26800VdVJ=800ln⁡3J≈878.890J.W_{\mathrm{qs}}=\int_2^6\frac{800}{V}dV\,\mathrm J=800\ln3\,\mathrm J\approx878.890\,\mathrm J.pf,qs=800/6=133.333kPa.p_{f,\mathrm{qs}}=800/6=133.333\,\mathrm{kPa}.The endpoints share volumes but need not share final thermodynamic states; the irreversible run can finish at 100 kPa if mechanical equilibrium is reached.

Physical check

An equilibrium pVpV curve is not automatically available during a strongly irreversible process.