The Molar Specific Heats of an Ideal Gas — Question 8

Section 19-7 · Physics pages 3166–3167

Question 8 Equal heat inputs do not imply equal final ideal-gas temperatures Use pV = nRT, R = 8.314 J/(mol K), and the sign convention ∆U = Q −W, with W the work done by the gas. Only pressure–volume work occurs. Two identical .200 mol samples begin at 300 K with CV = 3 2R. Each receives 249.42 J reversibly. A is held at fixed volume; B is held at fixed pressure. A: rigid vessel B: free piston Separate samples or species for comparison. (a) Find both final temperatures and the fraction of B heat stored internally. (b) If the two initial volumes are equal, compare the final pressures and volumes relative to their common initial values.
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Question 8 - Solution Equal heat inputs do not imply equal final ideal-gas temperatures A: rigid vessel B: free piston (a) Method and calculation ∆TA = 249.42 (.200)(1.50)(8.314) = 100 K ⇒TA = 400 K. ∆TB = 249.42 (.200)(2.50)(8.314) = 60.0 K ⇒TB = 360 K. ∆UB/QB = CV /Cp = 3/5. (b) Interpretation and further calculation pA/pi = TA/Ti = 4/3, VA/Vi = 1. pB/pi = 1, VB/Vi = TB/Ti = 6/5. B spends 40% of its heat on expansion, reducing its temperature rise relative to A. Physical check The same heat input creates different final states because the mechanical constraints differ.

Question 8

Equal heat inputs do not imply equal final ideal-gas temperatures

Use pV=nRTpV=nRT, R=8.314R=8.314 J/(mol K), and the sign convention ΔU=Q−W\Delta U=Q-W, with WW the work done by the gas. Only pressure–volume work occurs. Two identical .200 mol samples begin at 300 K with CV=32RC_V=\tfrac32R. Each receives 249.42 J reversibly. A is held at fixed volume; B is held at fixed pressure.

Diagram shown in the original SVG worksheet.

  1. Find both final temperatures and the fraction of B heat stored internally.

  2. If the two initial volumes are equal, compare the final pressures and volumes relative to their common initial values.

Question 8 - Solution

Equal heat inputs do not imply equal final ideal-gas temperatures

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΔTA=249.42(.200)(1.50)(8.314)=100K⇒TA=400K.\Delta T_A=\frac{249.42}{(.200)(1.50)(8.314)}=100\,\mathrm K\ \Rightarrow\ T_A=400\,\mathrm K.ΔTB=249.42(.200)(2.50)(8.314)=60.0K⇒TB=360K.\Delta T_B=\frac{249.42}{(.200)(2.50)(8.314)}=60.0\,\mathrm K\ \Rightarrow\ T_B=360\,\mathrm K.ΔUB/QB=CV/Cp=3/5.\Delta U_B/Q_B=C_V/C_p=3/5.

(b) Interpretation and further calculation

pA/pi=TA/Ti=4/3,VA/Vi=1.p_A/p_i=T_A/T_i=4/3,\quad V_A/V_i=1.pB/pi=1,VB/Vi=TB/Ti=6/5.p_B/p_i=1,\quad V_B/V_i=T_B/T_i=6/5.B spends 40% of its heat on expansion, reducing its temperature rise relative to A.

Physical check

The same heat input creates different final states because the mechanical constraints differ.