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 642: 19.35

Answer

(a) $n = 0.681 mol$ (b) $V_a = 0.0333 m^3 $ (c) $W = 2.23 kJ$ (d) $\Delta U = 0 $

Work Step by Step

(a) Moles of the gas. We use point b as the reference point. $n = \frac{p_bV_b}{RT_b} $ $n = \frac{(0.200 atm) (1.013 \times 10^5 Pa/atm)(0.100 m^3)}{(8.314 J/mol.K))(358K)} $ $n = 0.681 mol$ (b) Volume at a when n, R, and T are constant $V_a = V_b\frac{p_b}{p_a}$ $V_a = (0.10 m^3) \frac{0.200 atm}{0.600 atm}$ $V_a = 0.0333 m^3 $ (c) Work done from a to b $W = nRTln (\frac{V_b}{V_a})$ $W = (0.681) ((8.314 J/mol.K) (358 K) ln (\frac{0.100 m^3}{0.0333 m^3})$ $W = 2228 J = 2.23 kJ$ (d) The change of internal energy $\Delta U = n (\frac{3}{2} R)\Delta T$ In isothermal process, $\Delta T = 0$ So $\Delta U = n (\frac{3}{2} R)(0)$ $\Delta U = 0 $. There is no change of internal energy during this process.
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