Thermodynamics - Carnot efficiency

In summary: But you don't really need to use COP explicity. In all cases: W = Qh-Qc and for Carnot cycles, \Delta S = Q_c/T_c - Q_h/T_h = 0 so Qc/Qh = Tc/Th. Note W = Qh-Qc = Qc(Qh/Qc - 1) = Qc(Th/Tc-1)In this case you are given the amount of heat that must be removed from the cold reservoir (Qc). You can just use the above line to find W from Qc.
  • #1
Wellesley
274
3

Homework Statement


On a hot day a house is kept cool by an air conditioner. The outside temperature is 32°C and the inside temperature is 21°C. Heat leaks into the house at the rate of 9000 kcal/h. If the air conditioner has the efficiency of a Carnot engine, what is the mechanical power that it requires to hold the inside temperature constant?

The Attempt at a Solution



e= 1-294/305 = 0.036066

e=W/QH

Power = 9000 kCal/hour --> 37656000 J/hour --> 10460 J/s

.036066=W/10460 ---> W (really power)=377.426 J/s

This problem seems pretty straightforward...but the back of the book has an answer of 390 W, which is ~13 more J/s than my answer, so I must have made a mistake...yet there are only two equations, and one conversion! Is this a rounding error from the book?
 
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  • #2
I think you're right.
 
  • #3
Wellesley said:

Homework Statement


On a hot day a house is kept cool by an air conditioner. The outside temperature is 32°C and the inside temperature is 21°C. Heat leaks into the house at the rate of 9000 kcal/h. If the air conditioner has the efficiency of a Carnot engine, what is the mechanical power that it requires to hold the inside temperature constant?

The Attempt at a Solution



e= 1-294/305 = 0.036066

e=W/QH

Power = 9000 kCal/hour --> 37656000 J/hour --> 10460 J/s

.036066=W/10460 ---> W (really power)=377.426 J/s

This problem seems pretty straightforward...but the back of the book has an answer of 390 W, which is ~13 more J/s than my answer, so I must have made a mistake...yet there are only two equations, and one conversion! Is this a rounding error from the book?
The Coefficient of Performance is defined as:

[tex]COP = \frac{Q_c}{W} = \frac{Q_c}{Q_h-Q_c}[/tex]

which, for a Carnot refrigerator is:

[tex]COP = \frac{T_c}{T_h-T_c}[/tex]

In this case COP = 294/11 = 26.7

Since Qc = 9000 Kcal/hr (ie. heat removed from the cold reservoir) or 37680 kJ/hr or 10470 watts, W = Qc/COP = 10470/26.7 = 392 watts

AM
 
  • #4
Andrew Mason said:
The Coefficient of Performance is defined as:

[tex]COP = \frac{Q_c}{W} = \frac{Q_c}{Q_h-Q_c}[/tex]

which, for a Carnot refrigerator is:

[tex]COP = \frac{T_c}{T_h-T_c}[/tex]

In this case COP = 294/11 = 26.7

Since Qc = 9000 Kcal/hr (ie. heat removed from the cold reservoir) or 37680 kJ/hr or 10470 watts, W = Qc/COP = 10470/26.7 = 392 watts

AM

I looked through the thermodynamics whole chapter, and I couldn't find a single reference to this equation. Is it derived from the Carnot engine efficiency -> e=W/Q? Your solution makes sense, I'm just puzzled why the equation is not even in the book.

Thanks for responding. I'm glad I didn't submit the assignments yet...
 
  • #5
Wellesley said:
I looked through the thermodynamics whole chapter, and I couldn't find a single reference to this equation. Is it derived from the Carnot engine efficiency -> e=W/Q? Your solution makes sense, I'm just puzzled why the equation is not even in the book.

Thanks for responding. I'm glad I didn't submit the assignments yet...
Performance measurement depends on the function of the device.

Efficiency (output/input or W/Qh) is used for heat engines since it produces work from heat input. For heat pumps, which deliver heat by moving it from colder to warmer reservoirs, a coefficient of performance (COP) is used of Qh/W (output/input being heat output to work input). For a refrigerator, which inputs work to remove heat from a cold reservoir, the performance is measured by Qc/W (output/input or heat removed to work input).

But you don't really need to use COP explicity. In all cases: W = Qh-Qc and for Carnot cycles, [itex]\Delta S = Q_c/T_c - Q_h/T_h = 0[/itex] so Qc/Qh = Tc/Th. Note W = Qh-Qc = Qc(Qh/Qc - 1) = Qc(Th/Tc-1)

In this case you are given the amount of heat that must be removed from the cold reservoir (Qc). You can just use the above line to find W from Qc.

AM
 

FAQ: Thermodynamics - Carnot efficiency

What is the Carnot efficiency?

The Carnot efficiency is the maximum possible efficiency of a heat engine operating between two temperatures, given by the ratio of the temperature difference between the hot and cold reservoirs to the absolute temperature of the hot reservoir. It is a theoretical limit for the efficiency of any heat engine.

How is the Carnot efficiency calculated?

The Carnot efficiency can be calculated using the formula: efficiency = (Th - Tc) / Th, where Th is the temperature of the hot reservoir and Tc is the temperature of the cold reservoir. This formula assumes that both reservoirs are in thermal equilibrium.

What is the significance of the Carnot efficiency?

The Carnot efficiency is significant because it sets a limit on the efficiency of any heat engine. No real-world heat engine can achieve 100% efficiency, but the Carnot efficiency provides a benchmark for comparing the efficiency of different engines.

How does the Carnot efficiency relate to the Second Law of Thermodynamics?

The Carnot efficiency is a direct consequence of the Second Law of Thermodynamics, which states that heat cannot spontaneously flow from a colder body to a hotter body. This means that no heat engine can be 100% efficient, as some energy will always be lost as heat.

Can the Carnot efficiency be exceeded?

No, the Carnot efficiency cannot be exceeded. It is a theoretical limit that cannot be surpassed by any real-world heat engine. However, with advancements in technology and engineering, we can get closer and closer to reaching the Carnot efficiency in our heat engines.

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