Ideal Gas Law and Isobaric Processes

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SUMMARY

The discussion centers on the Ideal Gas Law and its application in isobaric processes, specifically addressing the relationship between temperature, pressure, and volume in a gas system. Participants clarify that while the Ideal Gas Law (PV = nRT) describes the state of an ideal gas, isobaric processes involve energy changes due to work done by the gas on its surroundings. The net energy change in an isobaric process is given by Esystem = q - Pext*V, indicating that work affects the system's internal energy and temperature. The conversation emphasizes the importance of understanding state changes and the role of enthalpy in simplifying energy calculations.

PREREQUISITES
  • Understanding of the Ideal Gas Law (PV = nRT)
  • Familiarity with isobaric processes and their characteristics
  • Knowledge of thermodynamic concepts such as internal energy and enthalpy
  • Basic principles of kinetic theory related to gas behavior
NEXT STEPS
  • Study the derivation and implications of the Ideal Gas Law in various thermodynamic processes
  • Learn about the First Law of Thermodynamics and its application to closed systems
  • Explore the concept of enthalpy and its relevance in isobaric processes
  • Investigate the combined gas law and its applications in real-world scenarios
USEFUL FOR

This discussion is beneficial for students and professionals in physics and engineering, particularly those focusing on thermodynamics, gas laws, and energy transfer in systems.

nothing123
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Hi,

So let's take the standard example of a gas in a container with a piston at the top. Charles' Law states that at constant pressure, an increase in temperature (kinetic energy of gas molecules) will increase the volume. This makes sense both conceptually and mathematically (per PV = nRT). However, in an isobaric process (pressure is constant again), the kinetic energy of the gas molecules is what is moving the piston so it must have lost some energy in doing so. Therefore, although initially Esystem = q that was added, it's net energy change would be Esystem = q - Pext*V.

So this is my problem, wouldn't this isobaric process be inconsistent with the ideal gas law? That is, using strictly the ideal gas law, woudn't the ending temperature not take into account the work done on the piston? Or are we assuming in using the ideal gas law that the work to keep the pressure constant is from an external source?

Thanks.
 
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nothing123 said:
Hi,

So let's take the standard example of a gas in a container with a piston at the top. Charles' Law states that at constant pressure, an increase in temperature (kinetic energy of gas molecules) will increase the volume. This makes sense both conceptually and mathematically (per PV = nRT). However, in an isobaric process (pressure is constant again), the kinetic energy of the gas molecules is what is moving the piston so it must have lost some energy in doing so. Therefore, although initially Esystem = q that was added, it's net energy change would be Esystem = q - Pext*V.

So this is my problem, wouldn't this isobaric process be inconsistent with the ideal gas law? That is, using strictly the ideal gas law, woudn't the ending temperature not take into account the work done on the piston? Or are we assuming in using the ideal gas law that the work to keep the pressure constant is from an external source?

Thanks.

You're mixing two different concepts. The ideal gas equation of state shows the relationship between P, V and T at a specified state. An isobaric process (or any process) shows how a substance changed from an initial state to a final state.

Does that help?

CS
 
Could you clarify exactly what you mean by states? I mean, since the heat added only changes the kinetic energy of the system (which is proportional to temperature), wouldn't we be able to find the same change in temperature whether we used Echange = q + w or whether we used T = PV/nR?

Thanks for your help so far.
 
nothing123 said:
Could you clarify exactly what you mean by states? I mean, since the heat added only changes the kinetic energy of the system (which is proportional to temperature), wouldn't we be able to find the same change in temperature whether we used Echange = q + w or whether we used T = PV/nR?

Thanks for your help so far.

By state I mean a set of properties that completely describe the condition of the system. If the system is not changing, it is in equilibrium. If the system undergoes a process, something has changed the system and it is now in an alternate state. The ideal gas law describes the state of an ideal gas. If the ideal gas undergoes a process, the process path from state 1 to state 2 will describe how the system changed. Once at state 2 the ideal gas relation can describe the system at that state.

Also, the properties of an ideal gas at two different states for a fixed mass are related by the ideal gas law as well and is called the combined gas law IIRC. However, you would need to know some of the properties at both states in order to solve for the unknown. Hence, the process path must be known.

BTW,

\Delta U = Q_{net,in} - W_{net,out}

Shows that for a closed system the internal energy of a substance decreases if it does work on it's surrounds. Hence it's temperature would decrease. So for an isobaric process like you described, the change in internal energy and thus temperature would depend on how much heat was added, and how much work was done by the piston on its surroundings.

This is typically stated using the enthalpy for simplicity:

Q - W_{other} = H_2 - H_1

Does that help?

CS
 
Thank you very much. Clearing up that state definition really helped.
 
nothing123 said:
Could you clarify exactly what you mean by states? I mean, since the heat added only changes the kinetic energy of the system (which is proportional to temperature), wouldn't we be able to find the same change in temperature whether we used Echange = q + w or whether we used T = PV/nR?

Thanks for your help so far.
T = PV/nR does not tell you the what P is and what V is. It only tells you what their product is. If T increases, PV must increase at the same rate. If it happens at constant volume, there is no work done by the gas. If it occurs at constant pressure, work is done so the heat flow is greater. PV=nRT always applies, as does dQ = dU + PdV.

AM
 

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