Thermodynamics - Carnot Cycle-esque question?

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SUMMARY

The discussion centers on calculating the efficiency of a reversible heat engine operating between an ideal gas and a heat reservoir. Given a mass of 9 kg of an ideal gas with specific heat capacity (cv) of 716 J/kgK and a gas constant (R) of 287 J/kgK, the initial conditions include a temperature (T1) of 772 K and a pressure (P1) of 106 Pa. The efficiency formula used is efficiency = (QH - QL)/QH, leading to a calculated efficiency of approximately 41.68%. The consensus confirms that at thermal equilibrium, the final temperature (T2) equals the reservoir temperature (THR) of 285 K.

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Homework Statement


A reversible heat engine produces work from the temperature difference that exists between a mass of m = 9 kg of an ideal gas (cv = 716 J/kgK, R = 287 J/kgK) in a rigid container and a heat reservoir at THR = 285 K. The only heat transfer interaction experienced by the container is with the heat engine. The gas in the container is initially at temperature T1 = 772 K and pressure P1 = 106 Pa. The reversible heat engine operates until the ideal gas and the heat reservoir are in thermal equilibirum (state 2). If the efficiency of the heat engine for process 1-2 can be defined as W/(QH)HE, calculate its value.Give your answer as a percent (without the % sign).

Homework Equations



  • efficiency = (QH - QL)/QH = W/QH
  • QL = MCvTHRln(T2/T1)
  • E2 - E1 = Q1-2 - W1-2
  • S2 - S1 = QL/ THR - change in entropy from or to a heat reservoir
  • QH = MCv(T2 - T1)

The Attempt at a Solution



If efficiency = (QH - QL)/QH[/B]
= 1 - (QL/QH)
= 1 - ((THRln(T2/T1))/(T2-T1))

I get an answer of 41.683538% but unsure as to what value to use for T2? Would I just use THR (Temp of heat reservoir) seeing as it works at thermal equilibrium? I used the temperature of the reservoir as the T2 value in my solution but not sure if this is correct?
 
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Somewhat amazingly I got the same answer! (I mean the final expression, not the % number. I don't do numbers!). Vote of confidence, anyway!
How can T2 be anything but the reservoir temperature THR? The reservoir has infinite heat capacity so at the end (i.e. "state 2") everything has to reach T = THR.
So far as I can see you got everything right. Congrats!
 

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