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 641: 19.15

Answer

(a)$W = 0 $ (b) $T_b = 2T_a$ (c) $ U_b = 700 J + U_a$

Work Step by Step

(a) The work done is calculated by $W = p(\Delta V)$ and in the figure, there is no change in volume so $\Delta V = 0$ $W = p(0)$ $W = 0 $ (b) The relationship between P and T is $pV = nRT$. During this process, heat is added and the pressure doubles in constant volume. $\frac{P}{T} = \frac{nR}{V}$ are constant so when P doubles, T also doubles $T_b = 2T_a$ (c) The change in internal energy is $\Delta U = \Delta Q - W$ $\Delta U = 700J - 0 $ $\Delta U = 700 J$ The internal energy at a and b is added together to result in $\Delta u$ $\Delta U = U_b - U_a$ $700 J = U_b - U_a$ $ U_b = 700 J + U_a$
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