(Zemansky & Dittman 5.14) An evacuated bottle with nonconducting walls is connected through a valve to a large supply of gas, where the pressure is Po and the temperature is To. The valve is opened slightly, and helium flows into the bottle until the pressure inside the bottle is Po. Assuming that the helium behaves like an ideal gas with constant heat capacities, show that the final temperature of the helium in the bottle is yTo.

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Chapter1: Units, Trigonometry. And Vectors
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(Zemansky & Dittman 5.14) An evacuated bottle with nonconducting walls is connected through a valve
to a large supply of gas, where the pressure is Po and the temperature is To. The valve is opened slightly,
and helium flows into the bottle until the pressure inside the bottle is Po. Assuming that the helium
behaves like an ideal gas with constant heat capacities, show that the final temperature of the helium in
the bottle is yTo.
Transcribed Image Text:(Zemansky & Dittman 5.14) An evacuated bottle with nonconducting walls is connected through a valve to a large supply of gas, where the pressure is Po and the temperature is To. The valve is opened slightly, and helium flows into the bottle until the pressure inside the bottle is Po. Assuming that the helium behaves like an ideal gas with constant heat capacities, show that the final temperature of the helium in the bottle is yTo.
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