A Closer Look at Heat and Work — Question 8

Section 18-8 · Physics pages 2966–2967

Question 8 Equal volume ratios give equal work along an isotherm A supplied ideal-gas model has pV = K = 600 J throughout a quasistatic constant-temperature expansion. It moves from 2.00 L to 8.00 L. Use W = ∫p dV . V p Schematic pressure–volume paths; work is the signed area under a process curve. (a) Find the work and the intermediate volume at which half the total work has been done. (b) Compare the work from 2 to 4 L with the work from 4 to 8 L. Explain why the halfway volume is not 5 L.
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Question 8 - Solution Equal volume ratios give equal work along an isotherm V p (a) Method and calculation W = K ∫Vf Vi dV V = K ln Vf Vi = 600 ln 4 ≈831.777 J. ln(Vm/Vi) = 1 2 ln(Vf/Vi) ⇒Vm = √ ViVf = 4.00 L. (b) Interpretation and further calculation W2→4 = 600 ln 2 = W4→8 ≈415.888 J. W2→5 W2→8 = ln(5/2) ln 4 ≈.66096. At 5 L more than half the work is already done because earlier volume increments occur at higher pressure. Physical check The logarithm acts on a dimensionless volume ratio; using litres or cubic metres gives identical work.

Question 8

Equal volume ratios give equal work along an isotherm

A supplied ideal-gas model has pV=K=600JpV=K=600\,\mathrm J throughout a quasistatic constant-temperature expansion. It moves from 2.00 L to 8.00 L. Use W=∫pdVW=\int p\,dV.

Diagram shown in the original SVG worksheet.

  1. Find the work and the intermediate volume at which half the total work has been done.

  2. Compare the work from 2 to 4 L with the work from 4 to 8 L. Explain why the halfway volume is not 5 L.

Question 8 - Solution

Equal volume ratios give equal work along an isotherm

Diagram shown in the original SVG worksheet.

(a) Method and calculation

W=K∫ViVfdVV=Kln⁡VfVi=600ln⁡4≈831.777J.W=K\int_{V_i}^{V_f}\frac{dV}{V}=K\ln\frac{V_f}{V_i}=600\ln4\approx831.777\,\mathrm J.ln⁡(Vm/Vi)=12ln⁡(Vf/Vi)⇒Vm=ViVf=4.00L.\ln(V_m/V_i)=\tfrac12\ln(V_f/V_i)\ \Rightarrow\ V_m=\sqrt{V_iV_f}=4.00\,\mathrm L.

(b) Interpretation and further calculation

W2→4=600ln⁡2=W4→8≈415.888J.W_{2\to4}=600\ln2=W_{4\to8}\approx415.888\,\mathrm J.W2→5W2→8=ln⁡(5/2)ln⁡4≈.66096.\frac{W_{2\to5}}{W_{2\to8}}=\frac{\ln(5/2)}{\ln4}\approx.66096.At 5 L more than half the work is already done because earlier volume increments occur at higher pressure.

Physical check

The logarithm acts on a dimensionless volume ratio; using litres or cubic metres gives identical work.