Work done in adiabatic quasistatic compression

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SUMMARY

The work done on 1 mole of a perfect gas during adiabatic quasistatic compression from volume V1 to V2 is calculated using the formula -∫(V1 to V2) P dV. The ideal gas law, P = nRT/V, is initially applied, leading to an incorrect result due to the assumption of constant temperature. The correct approach utilizes the relationship PV^γ = constant, acknowledging that temperature changes during adiabatic processes as internal energy varies with work done on the gas.

PREREQUISITES
  • Understanding of the ideal gas law
  • Knowledge of adiabatic processes in thermodynamics
  • Familiarity with calculus, specifically integration
  • Concept of internal energy and its relation to temperature for ideal gases
NEXT STEPS
  • Study the derivation of the adiabatic process equations
  • Learn about the first law of thermodynamics and its application to adiabatic processes
  • Explore the concept of heat capacity and its role in adiabatic transformations
  • Investigate the implications of the ideal gas law under non-constant temperature conditions
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Students and professionals in physics and engineering, particularly those focusing on thermodynamics and fluid mechanics, will benefit from this discussion.

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Hey!

"Calculate the work done on 1 mole of a perfect gas in an adiabatic quasistatic compression from volume V1 to V2."

The work done on the gas in this compression is:

<br /> -\int_{V1}^{V2} P dV<br />

Because we are talking about an ideal gas the ideal gas law applies so:

<br /> P=\frac{nRT}{V}<br />

Inserting this gives

<br /> -\int_{V1}^{V2} \frac{nRT}{V} dV = nRT Log[\frac{V1}{V2}]<br />

But for some reason this is not the correct result. However, I get the correct result if I use:

<br /> P V^\gamma = const<br />

What's going on? Why can't I use the ideal gas law?
 
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You have assumed that the temperature is constant and you pulled it out of the integral. But the temperature cannot be constant because there is no heat exchange with the environement, and so as work is done on the gaz, its internal energy changes. And for an ideal gaz, internal energy is directly linked to temperature:

E(T)=\frac{3}{2}\nu T
 
Hmm, of course... what was i thinking :-) Thanks a lot!
 

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