Ideal Gas in Cylinder with Piston (Conceptual)

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SUMMARY

The discussion centers on the behavior of an ideal gas in a cylinder with a piston when a valve is opened, allowing gas to escape while maintaining thermal equilibrium. It is established that during this quasistatic process, the internal pressure equilibrates with the external atmospheric pressure. The analysis employs the first law of thermodynamics, demonstrating that the heat transfer (Q) equals zero, indicating an adiabatic process under specific conditions. The final pressure of the gas inside the cylinder is less than the initial pressure due to the decrease in the number of moles (n) and volume (V) after gas escapes.

PREREQUISITES
  • Understanding of ideal gas laws and equations (PV=nRT).
  • Familiarity with the first law of thermodynamics.
  • Knowledge of quasistatic and adiabatic processes.
  • Basic principles of heat transfer and thermal equilibrium.
NEXT STEPS
  • Study the implications of the first law of thermodynamics in open systems.
  • Learn about the characteristics of quasistatic and adiabatic processes in thermodynamics.
  • Explore the concept of enthalpy and its role in thermodynamic processes.
  • Investigate the ideal gas law applications in real-world scenarios.
USEFUL FOR

Students and professionals in physics and engineering, particularly those focusing on thermodynamics, fluid mechanics, and heat transfer. This discussion is beneficial for anyone seeking to deepen their understanding of gas behavior in controlled environments.

fiestyman001
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You have a cylinder with an ideal gas inside, enclosed by a piston. There is a valve on the side of the cylinder could let gas through if opened. The valve is then opened and some of the gas escapes slowly while maintaining thermal equilibrium. Once it is closed, the piston is a little lower than it was before. Is the final pressure of the gas inside the cylinder greater, less than, or equal to the initial pressure?

I know n, and V change, but I'm not sure if P changes..
 
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Let me ask you this, what is causing the pressure in the cylinder?

Try a force balance on the piston, see if that answers your question.
 
Last edited:
fiestyman001 said:
You have a cylinder with an ideal gas inside, enclosed by a piston. There is a valve on the side of the cylinder could let gas through if opened. The valve is then opened and some of the gas escapes slowly while maintaining thermal equilibrium. Once it is closed, the piston is a little lower than it was before. Is the final pressure of the gas inside the cylinder greater, less than, or equal to the initial pressure?

I know n, and V change, but I'm not sure if P changes..

h2oski1326 observation is essential. Notice that the external forces exerted over the piston are its proper weight and the force due to atmospheric pressure. So if we assume a quasistatic process, then the internal pressure is equilibrated by the external one all the time during the process. Also to mantain thermal equilibrium (I assume, in advance, that the process is non-adiabatic as you are talking about of thermal equilibrium, but if the process were adiabatic then it is easy to show that it must be isentropic) some heat, in principle, should be transferred between the open system (control volume) and its surroundings. Furthermore, since T=const. and we are dealing with an ideal gas, the exit enthalpy may be asummed constant and equals to the system, that is h_e=C_p.T=const. But what n is? as in an isothermal process the polytropic constant is equal to 1. But I think n is the mole's number. So PV_1=m_1.R.T, and PV_2=m_2.R.T, where m_1 and m_2 are the initial and final mass resp. inside the control volume. Also by continuity eq. m_e=m_1-m_2. So by the first law of thermodynamics applied to a 'transitory' control volume
Q=m_e.h_e+m_2.u2-m_1.u_1+W,
where u_1=u_2=C_v.T, h_e=C_p.T. and W=-P(V_1-V_2), negative because work is efectued on the system by the piston.
Therefore,
Q=(m_1-m_2)C_p.T-(m_1-m_2)C_v.T-P(V_1-V_2)=(m_1-m_2)(C_p-C_v)T-P(V_1-V_2),
and we get
Q=(m_1-m_2)RT-P(V_1-V_2)=P(V_1-V_2)-P(V_1-V_2),
that is,
Q=0.
So, according to this result (and if I didn't commit mistakes), the process is also adiabatic in this very particular case. How much it is the entropy change?
 

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