Thermodynamics: Compression of an Adiabatic Gas

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SUMMARY

The discussion focuses on the compression of a monatomic ideal gas under adiabatic conditions. The initial pressure was calculated to be 11.6 atm and the final pressure 34.8 atm for a volume change from 3.00 L to 1.00 L at a constant temperature of 10.0 °C. The work input for a reversible isothermal process was determined to be 3.88 kJ. The participants clarified that in an adiabatic process, the heat transfer (q) is zero, leading to the relationship ΔU = -w, which is essential for solving the problem.

PREREQUISITES
  • Understanding of the Ideal Gas Law (PV=nRT)
  • Knowledge of thermodynamic processes, specifically isothermal and adiabatic processes
  • Familiarity with work calculations in thermodynamics (w=-nRTln(vf/vi))
  • Concept of internal energy change (ΔU) in thermodynamic systems
NEXT STEPS
  • Study the derivation and application of the adiabatic process equations
  • Learn about the First Law of Thermodynamics and its implications for work and heat transfer
  • Explore the concept of specific heat capacities for monatomic ideal gases
  • Investigate real-world applications of adiabatic processes in engineering systems
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Students in thermodynamics, mechanical engineers, and anyone studying the behavior of gases under varying pressure and temperature conditions.

Minescrushessouls
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Homework Statement


Assume 1.500 mol of a monatomic ideal gas is compressed from 3.00 L to 1.00 L.

a. If the initial and final temperature is 10.0 °C, what are the initial and final pressures (in atm)?

b. How much work input (in kJ) is required if a reversible isothermal path at 10.0 °C is followed?

c. How much work input (in kJ) is required if the compression is adiabatic rather than isothermal? Assume the initial temperature is 10.0 °C.

Homework Equations


PV=nRT
w=-nRTln(vf/vi)
U=q+w

The Attempt at a Solution


I got both a and b using the first two equations I listed. I got the inital pressure to be 11.6 atm and the final pressure to be 34.8 atm. For the second part I got the work to be 3.88 kJ.

I'm stuck on the third part. I know adiabatic means that there no change in U, so q=-w but I don't know how that applies to the question.
 
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You're missing an equation for the energy U of an ideal gas. And adiabatic does not mean ΔU = 0, it means q = 0.
 
So ΔU=-PΔV, where U=w

But the problem isn't isobaric, so that equation wouldn't work. I can't seem to find another equation though...
 

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