Thermodynamics problem: Adiabatic free expansion

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SUMMARY

The discussion centers on a thermodynamics problem involving adiabatic free expansion of nitrogen gas in a rigid, non-conducting tank. The initial conditions include a pressure of 3.1 bar and a temperature of 333.5 K for the nitrogen, occupying one-third of the tank's 4.6 m³ volume. The final pressure after the membrane ruptures is correctly calculated as 1.03 bar, with the conclusion that there is no change in temperature due to the adiabatic nature of the process. The confusion arose from the application of the adiabatic process equation, which is only valid for reversible processes, leading to an incorrect assumption about temperature change.

PREREQUISITES
  • Understanding of ideal gas laws and equations.
  • Knowledge of adiabatic processes and their characteristics.
  • Familiarity with heat capacities, specifically Cp and Cv for ideal gases.
  • Basic principles of thermodynamics, including internal energy changes.
NEXT STEPS
  • Review the principles of adiabatic processes and their applications in thermodynamics.
  • Study the differences between reversible and irreversible processes in thermodynamics.
  • Learn about the ideal gas law and its implications for gas behavior in various conditions.
  • Explore the derivation and application of internal energy equations, particularly ΔU = mCvΔT.
USEFUL FOR

Students and professionals in thermodynamics, mechanical engineers, and anyone studying gas behavior in adiabatic processes will benefit from this discussion.

nakamura25
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Homework Statement


A rigid ( ie. Constant volume), non-conducting ( ie. Perfectly insulated, no heat losses or gain) tank with a volume of 4.6 m^3. The tank is divided into two unequal parts by a thin membrane. One side of the membrane representing 1/3 of the tank is filled with nitrogen ( may be assumed to be an ideal gas) at 3.1 bar and 333.5 K. The other side of the membrane is evacuated. The membrane ruptures and the gas fills the entire tank. Heat capacity of nitrogen, Cp=3.5 R.
What is the final pressure of the gas in the tank?

The Attempt at a Solution


My thought was:
Non-conducting means adiabatic, hence Q = 0.
Free expansion, no external work, W = 0.
delta u = Q + W = Cp*(deltaT) = 0. So the temperature stays the same.
Since nitrogen can be assumed to be ideal gas, I used ideal gas law to calculated final pressure.
(P1)*(V1) = (P2)*(V2)
(3.1 bar)*(1/3)V = (P2)*(V)
P2 = 3.1/3 = 1.03 bar


Later on I saw this video lecture by UC Boulder:
http://www.learncheme.com/page/ideal-gas-expansion-closed
I think the question and result are the same for my case. So I summited my answer. But it turned out that the temperature does change, since the gas will do work to expand. Also, the final pressure should be 1.76 bar. I tried to use the adiabatic process equation p2/p1 = (V1/V2)^(Cp/Cv). Still could not get the right answer.

My questions are:
What's wrong with my reasoning? Does that mean the solution in the video is also wrong?
How to solve this problem for final pressure and temperature?

I'd really appreciate your effort. Any hint or solution would be helpful. Thank you.

Best Regards,
Naka
 
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The adiabatic process relationship you used is strictly for reversible process, which in this case the system is not. That's why you're getting the wrong answer
 
Also, it depends on what you choose as your system. If the whole entity inside the tank is the system then V is constant. Which means Work is zero...
 
Your original analysis was flawless. I like SN94's approach in post #3, taking the system as the entire contents of the tank. That certainly confirms that W = 0. So ΔU=0, and there is no change in temperature. And your calculation of the final pressure is correct. My only criticism if that you wrote down the equation for ΔU incorrectly. It should be ΔU=mCvdT, not Cp.

If your answer was marked wrong, whoever marked it wrong was incorrect.

Chet
 
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