Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 17 - Work, Heat, and the First Law of Thermodynamics - Exercises and Problems - Page 501: 82

Answer

$38.4\;\rm J$

Work Step by Step

We are given the following, $$P_1=\dfrac{F_{sp}}{A}=\dfrac{kx_1}{A}$$ where $x$ is the compressed distance by the spring and $A$ is the cross-sectional area of the piston. Hence, the final pressure is given by $$P_2 =\dfrac{kx_2}{A}$$ $$V_1=AL_1$$ and $$V_2=AL_2=A(L_1+\Delta L)$$ $$T_1=300\;\rm K$$ so the final temperature is given by $$\dfrac{P_1V_1}{T_1}=\dfrac{P_2V_2}{T_2}$$ Hence, $$T_2=\dfrac{P_2V_2T_1}{P_1V_1} $$ Plugging from the given; $$T_2=\dfrac{ (\frac{kx_2}{A})(AL_2)(300)}{(\frac{kx_1}{A})(AL_1)} =\dfrac{x_2L_2(300)}{x_1L_1} $$ where $x_1=2$ cm and after expanding the gas extra 6 cm, the spring will be compressed a distance of $x_2=6+2=8$ cm. $$T_2=\dfrac{ ( 0.08)( 0.16)(300)}{( 0.02)( 0.10)}=\bf 1920\;\rm K $$ Now we can find the change in the thermal energy of the system $$\Delta E_{th}=Q+W=nC_{\rm v}\Delta T$$ Hence, the heat energy needed is given by $$Q=nC_{\rm v}(T_2-T_1)-W\tag 1$$ Now we need to find the work done on the gas and the number of moles of the gas. $$n=\dfrac{P_1V_1}{RT_1}$$ Plugging the known; $$n=\dfrac{(\frac{kx_1}{A})(AL_1)}{RT_1} =\dfrac{kx_1L_1}{RT_1} $$ $$n=\dfrac{(2000)(0.02)(0.10)}{(8.31)(300)}=\bf 0.00160\;\rm mol$$ The work done on the gas is given by $$W=-\int PdV$$ where $P=kx/A$ and hence $dV=Adx$ $$W=-\int_{x_1}^{x_2} \dfrac{kx}{A}(Adx) =-k\int_{x_1}^{x_2} xdx$$ $$W=\dfrac{-kx^2}{2}\bigg|_{x_1}^{x_2}=\dfrac{-k}{2}(x_2^2-x_1^2)$$ Plugging the known; $$W =\dfrac{-2000}{2}(0.08^2-0.02^2)=\bf -6\;\rm J$$ Plugging all the known into (1); $$Q=(0.00160)(12.5)(1920-300)-(-6)=\color{red}{\bf 38.4}\;\rm J $$
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