Chemical Thermodynamics: Diagram-Based Questions (7)

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Question

A gas is taken through the cyclic process: A→B isobaric expansion, B→C isochoric pressure drop, C→A isothermal compression. Given TA=300T_A = 300 K, VA=1V_A = 1 L, PA=2P_A = 2 atm, and VB=2V_B = 2 L. Find ΔU\Delta U, WW, and QQ for the full cycle.

Solution — Step by Step

A: PA=2P_A = 2 atm, VA=1V_A = 1 L, TA=300T_A = 300 K.

A→B is isobaric, so PB=2P_B = 2 atm. VB=2V_B = 2 L. By ideal gas law: TB=TAVB/VA=600T_B = T_A \cdot V_B/V_A = 600 K.

B→C is isochoric, so VC=2V_C = 2 L. C→A is isothermal — meaning TC=TA=300T_C = T_A = 300 K. By ideal gas: PC=PAVA/VC=1P_C = P_A \cdot V_A/V_C = 1 atm.

A→B (isobaric): WAB=PΔV=2×1=2W_{AB} = P\Delta V = 2 \times 1 = 2 atm·L.

B→C (isochoric): WBC=0W_{BC} = 0.

C→A (isothermal): WCA=nRTln(VA/VC)=PAVAln(VA/VC)=(2)(1)ln(0.5)=2ln2W_{CA} = nRT \ln(V_A/V_C) = P_A V_A \ln(V_A/V_C) = (2)(1)\ln(0.5) = -2\ln 2 atm·L 1.386\approx -1.386 atm·L.

Wnet=2+01.386=0.614atm⋅L62.2JW_{net} = 2 + 0 - 1.386 = 0.614 \, \text{atm·L} \approx 62.2 \, \text{J}

(using 11 atm·L 101.3\approx 101.3 J)

ΔU=0\Delta U = 0 for a cycle (state function returns to start).

By first law: Qnet=ΔU+Wnet=0+62.2=62.2Q_{net} = \Delta U + W_{net} = 0 + 62.2 = 62.2 J.

Final answer: ΔUcycle=0\Delta U_{cycle} = 0, Wcycle62.2W_{cycle} \approx 62.2 J, Qcycle62.2Q_{cycle} \approx 62.2 J.

Why This Works

Internal energy depends only on state, so any closed cycle has ΔU=0\Delta U = 0. The first law ΔU=QW\Delta U = Q - W then gives Q=WQ = W for the cycle. The net work equals the area enclosed by the cycle on a PP-VV diagram.

This is true for any cycle, regardless of the working substance (ideal gas, real gas, refrigerant) — a powerful conceptual shortcut.

Alternative Method

Compute QQ for each segment using CpC_p and CvC_v, then sum. Slower but useful when individual segment heats are asked.

The area enclosed by a cycle on a PP-VV diagram equals the net work done. Clockwise = positive (heat engine). Anticlockwise = negative (refrigerator). This visual shortcut beats algebra in MCQs.

Forgetting the sign of WW in the isothermal compression. Volume decreases, so ln(Vf/Vi)<0\ln(V_f/V_i) < 0, making W<0W < 0 — gas absorbs work, not delivers it. Sign comes naturally from ln\ln, but only if you keep VfV_f on top.

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