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Q. If at $ 60 ^{\circ } C $ and $ 80\, cm $ of mercury pressure, a definite mass of a gas is compressed slowly, then the final pressure of the gas if the final volume is half of the initial volume $ (\gamma = 3/2) $ is

Thermodynamics

Solution:

Here, $ P_1 = 80 \,cm $ of $ Hg $ .
If the gas is compressed slowly, then the process is isothermal.
In this case $ P_1V_1 = P_2V_2 $
$ \therefore P_{2} =\frac{ P_{1}V_{1}}{V_{2}} $
$ = \frac{80\times V_{1}}{\frac{V_{1}}{2}} $
$ = 160\, cm $ of $ Hg \left(\because V_{2} =\frac{V_{1}}{2}\right) $