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 499: 54

Answer

a) $1.1\times 10^5\;\rm Pa$ b) $24.4\;\rm cm$

Work Step by Step

a) The piston is stationary which means that the net force exerted on it is zero. $$\sum F_y=P_{gas}A-P_{air}A-m_{piston}g =0$$ Noting that the gas pressure force affects upward while the air pressure affects downward. Thus, the gas pressure is given by $$P_{gas}=\dfrac{P_{air}A+mg}{A}=P_{air} +\dfrac{mg}{A}$$ $$P_{gas}= P_{air} +\dfrac{mg}{\pi r^2}$$ Plugging the known $$P_{gas}= (100\times 10^3) +\dfrac{(5.1)(9.8)}{\pi (4\times 10^{-2})^2}$$ $$P_{gas}=\color{red}{\bf 1.1 \times 10^5}\;\rm Pa$$ --- b) Since the piston is frictionless, the temperature of the gas is constant. This means that adding extra mass is making the gas undergoes an isothermal compression process. Thus, $$P_1V_1=P_2V_2$$ $$P_1Ah_1=P_2Ah_2$$ Hence, $$h_2=\dfrac{P_1h_1}{P_2}\tag 1$$ We found $P_1$ above in part (a) and now we need to find $P_2$. Using the same approach; $$P_{2}= P_{air} +\dfrac{m_{total}g}{\pi r^2}$$ $$P_{2}= P_{air} +\dfrac{(m_{piston}+m_{added})g}{\pi r^2}$$ Plugging the known; $$P_{2}= (100\times 10^3) +\dfrac{(5.1+3.5)(9.8)}{\pi (4\times 10^{-2})^2}$$ $$P_{2}= 1.17\times 10^5\;\rm Pa$$ Plugging into (1) $$h_2=\dfrac{(1.1 \times 10^5)(26) }{(1.17\times 10^5)} $$ $$h_2=\color{red}{\bf24.4}\;\rm cm$$
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