What Are the Work Relations for Different Processes in an Ideal Gas?

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SUMMARY

The discussion provides detailed equations for calculating work done on an ideal gas during various thermodynamic processes, including polytropic, isentropic, isobaric, and isothermal processes. The polytropic process is defined by the equation PV^n = constant, with the work done expressed as W = (m R (T2 - T1) / (1-n) = (P2 V2 - P1 V1) / (1-n). For isothermal processes, the work is calculated using W = mRT ln (V2/V1) = mRT ln (P1/P2). Specific values for the polytropic exponent (n) are provided for different processes, such as n = 0 for isobaric and n = 1 for isothermal.

PREREQUISITES
  • Understanding of thermodynamic processes
  • Familiarity with the ideal gas law
  • Knowledge of calculus for integration
  • Basic concepts of specific heats of gases
NEXT STEPS
  • Research the derivation of the ideal gas law and its applications
  • Learn about the implications of the polytropic process in real-world applications
  • Study the differences between isothermal and adiabatic processes
  • Explore the role of specific heats in thermodynamic calculations
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This discussion is beneficial for students and professionals in thermodynamics, mechanical engineers, and anyone involved in the study of gas behavior under various conditions.

blinder
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I was wondering if anyone knows where i can find the work relations for an ideal gas including isometric, isothermal, polytropic, isobaric, etc.
 
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Hi blinder. I'm assuming you're looking for the equations to calculate the work done on an ideal gas when undergoing the various processes you've listed. A polytropic process is the most general, so we can start with that. Also, the equations should work just as well for compression or expansion (work in or out of the gas).

As you must already know PV^n = constant is a polytropic process. If you compress a gas, the work done is the integral of PdV. If we integrate that for a polytropic process you end up with:

W = (m R (T2 - T1) / (1-n) = (P2 V2 - P1 V1) / (1-n)
where m = mass
R = Gas Constant
T = temperature
n = polytropic exponent
P = absolute pressure
V = total volume
(for any value of n except 1)

For an isentropic compression, n = the ratio of specific heats of the gas (ex: 1.667 for a monotomic gas, 1.4 for a diatomic gas, etc...)

For an isobaric process, n = 0

For an isothermal process, n = 1 so you need to do the integration using n=1 which comes out to:

W = mRT ln (V2/V1) = mRT ln (P1/P2)

Hope that helps.
 

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