University Physics with Modern Physics (14th Edition)

Published by Pearson
ISBN 10: 0321973615
ISBN 13: 978-0-32197-361-0

Chapter 19 - The First Law of Thermodynamics - Problems - Exercises - Page 640: 19.7

Answer

(a) $W_{net} = (p_1 - p_2 ) (V_2 - V_1)$ (b) $W_{net} = - (p_1 - p_2 ) (V_2 - V_1)$

Work Step by Step

(a) When P is constant, $W = p\Delta V$ So the total W for the whole system is $W_{13} + W_{32} + W_{24} + W_{41} $ Where $W_{13} = p_1(V_2 −V_1)$ $ W_{32} = 0 $ $W_{24} = p_2(V_1 −V_2) $ $W_{41} = 0 $ $W_{13} + W_{32} + W_{24} + W_{41} $ $W_{net} = p_1(V_2 −V_1) + p_2(V_1 −V_2) $ $W_{net} = p_1V_2 −P_1V_1 + p_2V_1 −p_2V_2 $ $W_{net} = (p_1 - p_2 ) (V_2 - V_1)$ If we observe, $W_{net} $ is the same as the area under the graph, in the closed loops. (b)For reverse process, the pressures are the same, but the volume changes are all the negatives of those found in part (a), so the total work is negative of the work found in part (a). $W_{net} = - (p_1 - p_2 ) (V_2 - V_1)$
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