Do All Engines Have the Same Efficiency as Carnot Engines?

In summary: ENSO it is not possible for an engine to be more efficient than a Carnot engine between the same two reservoirs. In summary, the quoted statement explains that no real heat engine can be more efficient than a Carnot engine and if two real engines are combined, it also violates the second law of thermodynamics. This means that any real or reversible engines operating between the same reservoirs will have the same efficiency, not just Carnot engines.
  • #1
annetjelie
3
0
My book states:

"To prove that no real heat engine operating between two reservoirs is more efficient than a carnot engine between the same reservoirs, imagine a more efficient engine to drive a less efficient carnot refrigerator. For the combination of the engine and refrigerator you get a net transfer of energy from the cold to the hot reservoir without work being done on the combination, which is a violation of the Clausius statement."

But what if i combine two *real* engines in the same way? This violates the Clausius statement too.
Does that mean that *any*(real or reversible) two or more engines between the same reservoirs have the same efficiency? I thought that was only true for Carnot engines.

help would be much appreciated, thanks in advance!
 
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  • #2
annetjelie said:
My book states:

"To prove that no real heat engine operating between two reservoirs is
more efficient than a carnot engine between the same reservoirs, imagine
a more efficient engine to drive a less efficient carnot refrigerator.
For the combination of the engine and refrigerator you get a net
transfer of energy from the cold to the hot reservoir without work being
done on the combination, which is a violation of the Clausius statement."

But what if i combine two *real* engines in the same way? This violates
the Clausius statement too.
Does that mean that *any*(real or reversible) two or more engines
between the same reservoirs have the same efficiency? I thought that was
only true for Carnot engines.
The quoted statement only leads to this conclusion if the refrigeration cycle is reversible. Here is the explanation:

Since the Carnot refrigerator cycle is reversible, after it delivers heat from the cold to the hot reservoir it can return to its original state by reversing the cycle and using the heat delivered to the hot reservoir to produce the same amount of work that was used in the cooling cycle (ie a Carnot engine). If that energy is stored, (eg. by raising a weight or stretching a spring) the cooling cycle can be repeated followed again by the engine cycle etc.ad infinitum.

But suppose the engine cycle (which takes the heat and produces work, which is stored and used to drive the Carnot refrigeration cycle) is more efficient than the Carnot cycle. This means that it produces MORE work with the heat Qh than the refrigerator cycle needs to deliver that Qh back to the hot reservoir. If the refrigerator then uses all of the engine's work output, it would deliver MORE heat than Qh from the cold reservoir back to the hot reservoir. This means the hot register would get hotter and the cold reservoir colder using no net energy (ie using the same energy over and over). And this violates the second law.

AM
 
  • #3


I would like to clarify that the statement in your book is correct. The Carnot engine, which operates between two reservoirs at different temperatures, is the most efficient engine possible. This is because it operates on the reversible Carnot cycle, which is the most efficient thermodynamic cycle possible.

When combining a more efficient engine with a less efficient Carnot refrigerator, you are essentially creating a perpetual motion machine, which is not possible according to the second law of thermodynamics. This is because the net transfer of energy from the cold to the hot reservoir without any work being done would violate the Clausius statement, which states that heat cannot flow from a colder body to a hotter body without any external work being done.

When combining two real engines in the same way, you are still violating the Clausius statement and creating a perpetual motion machine. This does not mean that any two real engines have the same efficiency, as the efficiency of a real engine depends on its design and operating conditions. However, the Carnot engine remains the most efficient engine possible, and any real engine will always have a lower efficiency than a Carnot engine operating between the same reservoirs.

I hope this helps clarify any confusion and reinforces the concept that the Carnot engine is the most efficient engine possible according to the laws of thermodynamics.
 

1. What is the Carnot cycle?

The Carnot cycle is a theoretical thermodynamic cycle that describes the most efficient operation of a heat engine. It is composed of four reversible processes: isothermal compression, adiabatic expansion, isothermal expansion, and adiabatic compression.

2. How does a real engine differ from a Carnot engine?

A real engine differs from a Carnot engine in several ways. First, real engines are not completely reversible and therefore cannot achieve the theoretical maximum efficiency of a Carnot engine. Additionally, real engines often experience losses due to friction, heat transfer, and other inefficiencies.

3. What is the Carnot efficiency?

The Carnot efficiency is the maximum efficiency that can be achieved by a heat engine operating between two constant temperature reservoirs. It is given by the ratio of the difference in temperature between the two reservoirs to the temperature of the hot reservoir.

4. What is the significance of the Carnot cycle in thermodynamics?

The Carnot cycle is significant because it serves as an ideal model for understanding the limitations of real engines and the principles of thermodynamics. It also provides a benchmark for comparing the efficiency of real engines and evaluating their performance.

5. How is the Carnot cycle related to the second law of thermodynamics?

The Carnot cycle is closely related to the second law of thermodynamics, which states that heat cannot spontaneously flow from a colder body to a hotter body. The Carnot cycle demonstrates that in order to achieve maximum efficiency, a heat engine must operate in a reversible manner, which is only possible in a theoretical, idealized system.

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