Heat engine: moles/temp unknown

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SUMMARY

The discussion focuses on calculating the efficiency of a heat engine using n moles of monatomic ideal gas in a closed cycle. The efficiency formula is derived from the work output (Wout) and heat input (QH), with the key equations being pV=nRT and efficiency = Wout/QH. The user initially calculated an efficiency of 84.1% but recognized errors in their approach regarding the heat involved in the isothermal and isochoric processes. Clarifications were made about the correct expressions for QH and the significance of temperature changes during the processes.

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  • Understanding of thermodynamic principles, particularly the behavior of ideal gases.
  • Familiarity with the first law of thermodynamics and efficiency calculations.
  • Knowledge of isothermal and isochoric processes in thermodynamics.
  • Ability to manipulate logarithmic expressions in the context of thermodynamic equations.
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  • Learn about the implications of isothermal and isochoric processes on heat transfer.
  • Explore the role of specific heat capacities (Cp and Cv) in thermodynamic calculations.
  • Investigate common mistakes in heat engine efficiency calculations and how to avoid them.
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joe_cool2
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Homework Statement



A heat engine uses the closed cycle shown in the diagram below. (Figure 1) The working substance is n moles of monatomic ideal gas. Find the efficiency of such a cycle. Use the values for pressure and volume shown in the diagram, and assume that the process between points 1 and 3 is isothermal.

1065003.jpg


Homework Equations



pV=nRT
efficiency = Wout/QH

The Attempt at a Solution



We know that T3 and T1 are on an isotherm, and so are both exactly 3 times T2. So, the absolute value of ΔT is 2 times T2. The reason I refer to the absolute value here is because the sign of ΔT for different processes will be different.

Wout = nRT*ln(V1/V3) - pΔV

So, Wout = nRT*ln(V1/V3) - nRΔT

QH= nRT*ln(V1/V3) + nCvΔT

So the efficiency is:

3nRT2*ln(V1/V3) + 2nRT2 / 3nRT2*ln(V1/V3) + 2nCVT2

Then the idea is to cancel out all the n's and T2's. All the rest are knowns. I get a value of 84.1%. There's definitely something very wrong about my approach.
 
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Did you consider the heat involved in 1->2?

I don't understand the last, long expression and I think there are brackets missing.
 
The heat involved in 1 -> 2 is actually leaving the system. So, QH is just the heat we put in during the isothermal and isochoric legs. So, the heat associated with the isobaric process, nCPΔT, does not enter into the expression for QH.

Yes, there were brackets missing. Let me clarify as to where this expression comes from.

[3nRT2*ln(V1/V3) + 2nRT2] / [3nRT2*ln(V1/V3) + 2nCVT2]

We know that T3 is three times greater than T2. This should help to explain the first term of the numerator and the first term of the denominator. The former is the heat intake during the isothermal process, and the latter is the work done during the isothermal process. These expressions are the same because in an isothermal process, W = QH.

The expression begins as nRT*ln(V1/V3). Now T can refer to the temeperature at point 1 or point 3, because we are dealing with an isothermal process. And we said in the last paragraph that 3T2 = T3. So this is where the 3T2 comes from in both expressions.

The second terms in the numerator and the denominator contain the factor 2T2. That's because ΔT = T3 - T2, so ΔT = 3T2 - T2.

Note the sign change on the second term in the numerator. That occurs because we lose temperature moving from 1 -> 2, so ΔT is negative. ΔT is not negative in the other place it occurs, moving from 2 -> 3.

EDIT: Let's not get trapped in the paradigm of my thinking. It hasn't gotten me anywhere with this problem.
 

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