Efficiency Calculation for a Stirling Engine Cycle

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Homework Help Overview

The discussion revolves around the efficiency calculation of a Stirling engine cycle, specifically analyzing the thermodynamic processes involved in the cycle as described in a provided figure. The problem involves an ideal monatomic gas undergoing isothermal and isochoric processes, with participants exploring the heat transfer and work done throughout the cycle.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the calculations for heat transfer (Q) and work (W) during different steps of the Stirling engine cycle. There is a focus on the relationship between work and heat in cyclic processes, with one participant questioning the validity of their efficiency calculation resulting in a value of 1.

Discussion Status

The discussion is ongoing, with participants providing detailed calculations for different steps of the cycle. One participant expresses confidence in their calculations for heat transfer but questions the efficiency result. Another participant suggests that the relationship between heat and work in cyclic processes supports their findings, indicating a productive exploration of the topic.

Contextual Notes

Participants are working within the constraints of a homework assignment, which may impose specific methods or formulas for calculating efficiency. There is an emphasis on ensuring that assumptions and definitions used in the calculations are scrutinized.

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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:
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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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