Efficiency Calculation for a Stirling Engine Cycle

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SUMMARY

The discussion focuses on the efficiency calculation of a Stirling engine cycle, specifically analyzing a thermodynamic model involving an ideal monatomic gas. The calculations for heat transfer (Q) and work (W) during the cycle reveal that the total heat transfer is 2nRTiLn(2) and the total work done is also 2nRTiLn(2). Consequently, the efficiency of the engine is calculated to be 1, indicating a perfect conversion of heat to work, which is theoretically possible in an ideal scenario.

PREREQUISITES
  • Understanding of thermodynamic cycles, specifically Stirling engines.
  • Familiarity with ideal gas laws and equations of state.
  • Knowledge of isothermal and isochoric processes.
  • Proficiency in calculating work and heat transfer in thermodynamic systems.
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  • Study the principles of Stirling engine design and operation.
  • Learn about the implications of ideal gas behavior in thermodynamic cycles.
  • Explore the derivation of efficiency formulas for various thermodynamic cycles.
  • Investigate real-world applications and limitations of Stirling engines in energy conversion.
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Students of thermodynamics, mechanical engineers, and anyone interested in the principles of heat engines and their efficiencies.

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Homework Statement



Figure 2 represents a model for the thermodynamic
cycle of the Stirling engine, patented by Scottish clergyman Robert Stirling in
1816. The engine operates by burning fuel externally to warm one of its two
cylinders. A xed quantity of inert gas moves cyclically between the cylinders,
expanding in the hot one and contracting in the cold one.

(a) Consider n mol of an ideal monatomic gas being taken
once through the cycle in Fig. 2, consisting of two isothermal processes
at temperatures 3Ti and Ti and two isochoric processes. In terms of n,
R, and Ti, determine Q for the complete cycle.

(b) What is the eciency of the engine? (Hint: The heat QH
transferred into the system happens during steps 1 and 4).

Figure 2:
f5PXbGE.png


Homework Equations



Work = nRT ln(v2/v1)
U = n Cv T
efficiency = W/Q

The Attempt at a Solution


I am pretty confident in my solution to part a ) of the problem which is this:
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However when it comes to calculating efficiency, I am getting an answer of 1 . Is this possible?

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Thank you.
 
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Whenever you're free try typing these equations use this
 
Okay,
So for a)

$$ Step \, 1-2\,$$
$$ Isothermal \, \therefore \delta U=0 \, , W=Q$$
$$W=nR3T_iLn(2V/V) \implies Q= nR\cdot3T_iLn(2)$$

$$Step \, 2-3 $$
$$Isochoric, \, W=0 $$
$$\delta U=n \frac{3}{2}R (T_i-3T_i) \implies Q=-2T_in\frac{3}{2}R $$

$$Step \, 3-4 $$
$$ Isothermal \, \therefore \delta U=0 \, , W=Q$$
$$W=nR3T_iLn(1V/2V) \implies Q= nR\cdot3T_iLn(1/2) = -nR\cdot3T_iln(2)$$

$$Step \,4-1$$
$$Isochoric, \, W=0 $$
$$\delta U=n \frac{3}{2}R (3T_i- T_i) \implies Q= 2T_in\frac{3}{2}R $$

$$Q_{total} = 2T_in\frac{3}{2}R + -nR\cdot3T_iln(2) + -2T_in\frac{3}{2}R + nR\cdot3T_iLn(2) = 2nRT_iLn(2) $$

$$W_{total} = nR3T_iLn(2) + 0 + nR3T_iLn(1/2) + 0 = 2nRT_iLn(2)$$

Part b)
$$ efficiency = \frac{W}{Q_H} = \frac{2nRT_iLn(2)}{2nRT_iLn(2)} = 1 $$
 
I would also like to add that this does make sense since for a cyclic process, $$\delta U = 0 = Q-W $$ and since Q=w, this holds. So,the question now is did I use the correct efficiency formula?
 

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