Comparing Work Output in 200K/300K and 300K/200K Environments

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Homework Help Overview

The discussion revolves around comparing the work output from two setups involving bricks at different temperatures in contrasting environments: a 200K brick in a 300K environment and a 300K brick in a 200K environment. Participants explore the implications of thermodynamic principles, particularly in the context of Carnot engines, while assuming equal mass and heat capacity for both bricks.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the integration of equations related to heat flow and efficiency, with some questioning the signs and variables used in their calculations. There is an exploration of how temperature differences affect work output in each scenario.

Discussion Status

The discussion is active, with participants sharing their calculations and reasoning. Some express confusion regarding the correct interpretation of the setups, while others offer insights into the underlying thermodynamic principles. There is a recognition of differing perspectives on which setup yields more work, indicating a lack of consensus.

Contextual Notes

Participants note the importance of careful consideration of heat flow and temperature changes in each case, as well as the potential for misinterpretation of the problem's requirements regarding work versus efficiency.

golanor
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Homework Statement


We have two different set ups:
a) A 200K brick in a 300K environment
b) A 300K brick in a 200K environment
From which one of these can you extract more work?
Assume equal mass and heat capacity.

Homework Equations


Efficiency - η=\frac{T_H - T_L}{T_H}
and:
W = ΔQ => W≤Q_H * \eta_C

The Attempt at a Solution


I regard both as cases as infinitesimal carnot engines.
a) T_L is varying, and after integration I get m*c*16.67 (m and c are the mass and heat capacity)
b) T_H is varying, after integration the result is m*c*19.
therefore, I conclude that i can get more work from b.
The problem is that the correct answer is marked a.
Anyone has an idea what i am doing wrong?
 
Last edited:
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You have the right approach (infinire sum of infinitesimal reversible cycles) but you have not shown your work so we can't help yoiu until you do.

Careful with the signs of dQ and dT in (a) and (b). I would go with dQ > 0 always but dT < 0 in (b).
 
Sorry, guess I was kind of lazy with copying it.
a)
\int_{200}^{300} {\frac{300 - T}{300}}{dT} = 100 - 250/3 = 16.67
b)
\int_{300}^{200} {\frac{T - 200}{T}}{dT} = -100 + 200 * \log(3/2) = 19
 
You'll have to derive the integral in (a), for starters. it's close but not what I got. Check the denominator! I got > 19.(b) I got the same as you.
 
golanor said:
Sorry, guess I was kind of lazy with copying it.
a)
\int_{200}^{300} {\frac{300 - T}{300}}{dT} = 100 - 250/3 = 16.67
b)
\int_{300}^{200} {\frac{T - 200}{T}}{dT} = -100 + 200 * \log(3/2) = 19
Maybe I'm missing something but I get your answers.
In fact, it seemed to me straight away that the answer is (b). At each point in time, the temperature difference between brick and environment is the same, but in (a) the overall temperature is higher. So you must be getting more work from (b).
 
haruspex said:
Maybe I'm missing something but I get your answers.
In fact, it seemed to me straight away that the answer is (b). At each point in time, the temperature difference between brick and environment is the same, but in (a) the overall temperature is higher. So you must be getting more work from (b).

Well, you saw my post. Do you want to compare notes privately?
 
I don't think you have to do any calculation here.

The real issue is how to extract work with the least amount of change in temperature difference per cycle. The first Carnot cycle will produce the same amount of work in either case. But in a) (the brick is receiving heat flow Qc) the heat flow to the brick (bringing the brick's temperature closer to surroundings by ΔT = Qc/Cv) is less than the heat flow from the brick in b) (bringing the brick's temperature closer to the surroundings by ΔT = Qh/Cv). So the next cycle will produce a bit more work in a) than in b) and so on.

AM
 
Last edited:
Andrew Mason said:
The real issue is how to extract work with the least amount of change in temperature difference per cycle. The first Carnot cycle will produce the same amount of work in either case. But in b) the heat flow to the brick (bringing the brick's temperature closer to surroundings by ΔT = Qc/Cv) is less than the heat flow from the brick in a) (bringing the brick's temperature closer to the surroundings by ΔT = Qh/Cv). So the next cycle will produce a bit more work in b) than in a) and so on.

AM

In part (a) heat is added to the brick.

I'm getting that the work in part (a) is greater than in (b), in line with rude man.
 
TSny said:
In part (a) heat is added to the brick.

I'm getting that the work in part (a) is greater than in (b), in line with rude man.
Yeah. Sorry about that. The reasoning in my earlier post was correct but I had in my mind a and b reversed. I have corrected it.

AM
 
  • #10
TSny said:
In part (a) heat is added to the brick.

I'm getting that the work in part (a) is greater than in (b), in line with rude man.

Yes, I agree. I had allowed myself to be misled by the efficiency calculation in posts 1 and 3. My argument in favour of (b) only leads to the conclusion that the efficiency is greater.
Reading the whole question, I see it asks for the work extracted, not the efficiency in doing so.
There's no contradiction, since the heat flow is greater in (a).
 

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