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 644: 19.53

Answer

(a) $Q = 450 J $ (b) $W = -450J$ (c) $\Delta U = 675 J$

Work Step by Step

(a) If the gas is isothermal, $\Delta T = 0$ so $\Delta U = nC_VΔT = 450 J $ Hence $Q = ΔU +W $ $Q = 0 + 450 J $ $Q = 450 J $ (b) For adiabatic, $Q = 0$ $0 = +450J +W $ $W = -450J$ Hence, $\Delta U = W = -450J$ (c) For isobaric, the pressure is constant, $\Delta V = 0$ We take $W = p\Delta V = nR \Delta T $ So $\Delta T = \frac{p \Delta V}{nR} = \frac{W}{nR}$ Now $Q = n\frac{5}{2}R \Delta T$ $Q = n\frac{5}{2}R(\frac{W}{nR})$ $Q = \frac{5}{2} W$ $Q = \frac{5}{2} (450 J)$ $Q = 1125 J $ Thus, $\Delta U = Q - W $ $\Delta U = 1125 J - 450 J $ $\Delta U = 675 J$
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