What is the Work Done on an Ideal Gas Under Isothermal Compression?

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SUMMARY

The work done on an ideal gas during isothermal compression can be calculated using the relationship P = AV, where A is a constant. The gas is compressed from an initial volume V1 to a final volume V2, which is half of V1. The work done, W, is derived from the integral of -PdV, resulting in W = -3nRT1/8. This formula incorporates the number of moles (n), the ideal gas constant (R), and the initial temperature (T1).

PREREQUISITES
  • Understanding of the ideal gas law (PV = nRT)
  • Familiarity with calculus, specifically integration techniques
  • Knowledge of isothermal processes in thermodynamics
  • Concept of reversible processes in gas dynamics
NEXT STEPS
  • Study the derivation of work done in isothermal processes using calculus
  • Learn about the implications of the ideal gas law in different thermodynamic processes
  • Explore the relationship between pressure, volume, and temperature in gas laws
  • Investigate advanced topics in thermodynamics, such as entropy and enthalpy
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Students returning to physics, thermodynamics enthusiasts, and anyone seeking to understand the principles of work done on gases during compression processes.

djaymilla
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An ideal gas originally at a temperature T1 and pressure P1 is compressed recersibly against a poston to a volume equal one-half of its original volume. The temperature of the gas is caried during the compression so that at each instant the relatoion P=AV is satisfied, where A is constant. Find the word done on the gas in terms of n, R, and T1.


PV=nRT
P=AV
AV^2=RT
dW= -PdV
W= - (integral from V1 to V2) PdV


I have the answer: [-3nRT1/8] but I cannot figure out how it is derived. I have tried using the work equation for an isothermal equation as well: W=nRT (integral from V1 to V2) dV/V where W=nRT ln (V2/V1)
 
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Hi djaymilla, welcome to PF. Why not just evaluate the work integral, plugging in AV for P?
 
Hey Mapes, thanks for the welcome. I guess I am confused with this problem because I don't have concrete terms with which to integrate. I'm not sure how to carry out the integral...

(sorry, this may seem elementary, but I'm now going BACK to school, and have been out of the physics/calculus game for quite some time)
 
You're almost there. You will need to integrate AV dV from V1 to V2, where A, V1, and V2 are constants. I'm sure you'll be able to figure this out. The remaining steps consist of expressing V2 in terms of V1 (you already described this relationship) and expressing V1 (more precisely, V1^2, hint hint) in terms of T1. Good luck.
 

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