Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 17 - Work, Heat, and the First Law of Thermodynamics - Exercises and Problems - Page 499: 57

Answer

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Work Step by Step

$\bullet\bullet $ In path A, the gas undergoes two processes: ​An isochoric process, then an expansion isobaric process. So, $$(\Delta E_{th})_A=W_A+Q_A\tag 1$$ $\bullet\bullet $ In path B, the gas undergoes two processes: ​An expansion isobaric process, then an isochoric process. $$(\Delta E_{th})_B=W_B+Q_B\tag 2$$ Since the two paths start and end at the same points, then $$(\Delta E_{th})_A=(\Delta E_{th})_B$$ Plugging from (1) and (2); $$W_A+Q_A=W_B+Q_B$$ Hence, $$Q_A-Q_B=W_B-W_A\tag 3$$ From the given graph, we can see that $$W_A=W_1+W_2=0+(-2P_i\Delta V)$$ $$W_A=- 2P_i(2V_i-V_i)=\boxed{-2P_iV_i}$$ And that $$W_B=W_1+W_2= -P_i\Delta V+0$$ $$W_B= -P_i(2V_i-V_i)=\boxed{- P_iV_i}$$ Plugging into (3); $$Q_A-Q_B=-P_iV_i-(-2P_iV_i)$$ $$\boxed{Q_A-Q_B=P_iV_i}$$
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