Entropy Change in a Carnot Engine

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Homework Help Overview

The discussion revolves around a Carnot engine operating between two thermal reservoirs at temperatures of 1000K and 280K, with a work output of 1kJ per cycle. Participants are exploring the efficiency of the engine and the entropy change of the gas during the heat transfer at the hot reservoir.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the calculation of efficiency and question the relationship between heat input and work output. There is uncertainty regarding the entropy change and how to account for energy rejected to the cold reservoir. Some participants suggest that the question may be asking for the entropy change due to heat absorption alone, while others seek clarification on the definitions of Q_1 and Q_2 in the context of the equations provided.

Discussion Status

The conversation is ongoing, with various interpretations being explored. Some participants have offered insights into the nature of the entropy change and the significance of the Carnot cycle's stages. There is no explicit consensus, but guidance has been provided regarding the relationship between efficiency, work, and heat flow.

Contextual Notes

Participants note that the change in entropy of the gas over a complete cycle is zero, raising questions about the specific focus of the problem. The discussion includes considerations of how to derive values for Q_1 and Q_2 based on the given efficiency and work output.

lms_89
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Homework Statement


A Carnot engine using a gas operates between 2 reservoirs of temperatures 1000K and 280K. The work output per cycle is 1kJ.
a) What is the efficiency?
b) What is the entropy change of the gas per cycle due to the heat transfer at the hot reservoir?

Homework Equations



[tex]\eta_{carnot} = 1 - \frac{Q_{1}}{Q_{2}} = 1 - \frac{T_{1}}{T_{2}}[/tex]

[tex]\Delta S = \int \frac{dQ}{T}[/tex]

[tex]\Delta U = W_{on} + Q_{in}[/tex]

The Attempt at a Solution


a) Seems easy enough, I got 72%.
b) I think you just use the entropy formula above, which goes to S = Q_in / T_2 (never used Latex before, and wasn't working here - don't have time to work out why!). If internal energy, U, is zero then heat in equals negative work done on the gas (ie. -1kJ) due to the 1st law. In that case I get the change in entropy to be 1.. which just doesn't seem right. Can anyone comment/help?

Thanks!
 
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I'm curious about what answer would "seem right"... OK, does heat in really equal work out? Isn't some energy also rejected to the cold reservoir?
 
I guess I'm not sure what answer would 'seem right'!

Perhaps some energy does go to the cold reservoir, but I don't know how you would do that. This is a past exam question on the 'easy'/bookwork section of the paper designed to get everyone some marks, so the questions are generally quite simple, so I get the feeling that needing to take the cold reservoir into account would make the question too complicated :confused:
 
lms_89 said:
Perhaps some energy does go to the cold reservoir, but I don't know how you would do that.

What are [itex]Q_1[/itex] and [itex]Q_2[/itex] in the equation you wrote?
 
Mapes said:
What are [itex]Q_1[/itex] and [itex]Q_2[/itex] in the equation you wrote?

I used the temperatures to calculate the efficiency, just wrote down the Q version of the formula because I thought it might be relevant, but am not sure how you can use it considering you know neither of the values. Obviously you can say Q_1/Q_2 = T_1/T_2 = 0.28 though.
 
Part b) is a rather odd question. The change in entropy of the gas in one cycle is 0 since it returns to its original state after a complete cycle. That occurs whether or not it is a Carnot cycle. So the question must be asking: what is the change in entropy resulting from the absorption of heat from the hot reservoir only, without regard to the rest of the cycle.

Since a Carnot cycle uses 1. isothermal heat absorption followed by 2. adiabatic expansion, then 3. isothermal heat release and finally 4. adiabatic compression, you are asked only for the change of entropy in 1 (as it is the only part in which heat flowed into the gas). To find that, all you have to know is Qh. You get that from the efficiency and the work output that is given.

AM
 
Andrew Mason said:
Part b) is a rather odd question. The change in entropy of the gas in one cycle is 0 since it returns to its original state after a complete cycle. That occurs whether or not it is a Carnot cycle. So the question must be asking: what is the change in entropy resulting from the absorption of heat from the hot reservoir only, without regard to the rest of the cycle.

Since a Carnot cycle uses 1. isothermal heat absorption followed by 2. adiabatic expansion, then 3. isothermal heat release and finally 4. adiabatic compression, you are asked only for the change of entropy in 1 (as it is the only part in which heat flowed into the gas). To find that, all you have to know is Qh. You get that from the efficiency and the work output that is given.

AM

What is your h representing? Also though I have Q_1 and Q_2, so which would it be and how would I get it from the efficiency since surely I only know the ratio of the two Q values?

Thanks both of you for your help so far, by the way.
 
Andrew Mason said:
So the question must be asking: what is the change in entropy resulting from the absorption of heat from the hot reservoir only, without regard to the rest of the cycle.

Definitely.

lms_89 said:
Also though I have Q_1 and Q_2, so which would it be and how would I get it from the efficiency since surely I only know the ratio of the two Q values?

You also know the difference between the two values. Of the energy coming in, what isn't sent to the cold reservoir must be output as work.
 
lms_89 said:
What is your h representing? Also though I have Q_1 and Q_2, so which would it be and how would I get it from the efficiency since surely I only know the ratio of the two Q values?

Thanks both of you for your help so far, by the way.
The efficiency is W/Qh. So you can easily find Qh given efficiency and W. With Qh and T you can work out the entropy. (I am using Qh as the heat flow from the hot reservoir).

AM
 

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