Efficiency Calculation for a Stirling Engine Cycle

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The discussion focuses on calculating the efficiency of a Stirling engine cycle using thermodynamic principles. The user successfully determines the heat transfer (Q) for the complete cycle involving isothermal and isochoric processes, resulting in a total heat of 2nRTiLn(2). However, they encounter an issue calculating the engine's efficiency, arriving at a value of 1, which raises questions about its validity. The user confirms that their calculations align with the principles of cyclic processes, where the change in internal energy equals zero. The discussion ultimately seeks clarification on whether the efficiency formula was applied correctly.
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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?
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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