Physics (10th Edition)

Published by Wiley
ISBN 10: 1118486897
ISBN 13: 978-1-11848-689-4

Chapter 14 - The Ideal Gas Law and Kinetic Theory - Problems - Page 385: 35

Answer

$3.9\times10^{5}J$

Work Step by Step

Here we use equation 14.7 $U=\frac{3}{2}nRT$ to find the increase in the internal energy of the gas. $\Delta U=U_{f}-U_{i}=\frac{3}{2}nRT_{f}-\frac{3}{2}nRT_{i}=\frac{3}{2}nR(T_{f}-T_{i})-(1)$ Let's apply the ideal gas law $PV=nRT$ to the initial state of the gas. $P_{i}V=nRT_{i}=>nR=\frac{P_{i}V}{T_{i}}-(2)$ (2)=>(1), $\Delta U=\frac{3}{2}\frac{P_{i}V}{T_{i}}(T_{f}-T_{i})$ ; Let's plug known values into this equation. $\Delta U=\frac{3(1.01\times10^{5}Pa)(680\space m^{3})}{2(293.2\space K)}(294.3\space K-293.2\space K)=3.9\times10^{5}J$ Increase in the internal energy of the gas = $3.9\times10^{5}J$
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