Is Carnot engine the only reversible engine?

Click For Summary

Discussion Overview

The discussion revolves around the nature of reversible engines, specifically questioning whether the Carnot engine is the only form of reversible engine and exploring the potential for other reversible engines, such as those based on the Otto cycle. Participants examine the implications of isochoric processes in the Otto cycle and their relationship to the second law of thermodynamics.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that the isochoric processes in the Otto cycle could theoretically be reversible, questioning if this means the Otto cycle could achieve the same efficiency as the Carnot cycle.
  • Others argue that the second law of thermodynamics implies that the Otto cycle cannot be reversible due to the entropy increase associated with heat dissipation to the surroundings.
  • A participant suggests that if different temperature reservoirs are used continuously, the Otto cycle could be modeled, but challenges the idea of drawing it on a P-V diagram due to the nature of irreversible processes.
  • Some participants assert that the Carnot engine is not the only reversible engine, and express agreement with the analysis of the situation regarding entropy changes in the reservoirs.
  • Questions arise about how to compare the efficiency of the Carnot engine with that of the ideal Otto engine, particularly given the complexity of multiple reservoirs in the Otto cycle.
  • Participants discuss deriving efficiency equations for the Otto cycle, noting that it may only be possible to express efficiency in terms of temperature ratios rather than exact temperatures due to the involvement of multiple reservoirs.

Areas of Agreement / Disagreement

Participants express differing views on the reversibility of the Otto cycle and its comparison to the Carnot cycle. There is no consensus on whether the Otto cycle can be considered reversible or on the implications of using multiple temperature reservoirs for efficiency calculations.

Contextual Notes

Participants highlight limitations in defining the efficiency of the Otto cycle due to the presence of multiple heat reservoirs and the lack of criteria for selecting a representative reservoir. The discussion also reflects uncertainty regarding the implications of the second law of thermodynamics on the reversibility of different cycles.

kelvin490
Gold Member
Messages
227
Reaction score
3
Is Carnot engine the only form of reversible engine? Is it possible to have a different form of reversible engine that goes through different processes?

For a standard Otto cycle working with ideal gas, theoretically the two processes involving isochoric pressure change can be reversible processes. Does it mean that the Otto cycle can also have same efficiency as Carnot cycle? Since temperature of the working fluid is changing during isochoric pressure change, does it mean there are infinite number of heat reservoirs being used at different temperatures so that there is no finite temperature difference at every point of the isochoric process?
 
Science news on Phys.org
The second law of thermodynamics states that the entropy of the universe continuously goes on increasing. Even though the system may arrive at the same state after every cycle, the heat dissipated to the surroundings during the isochoric expansion increases the entropy of the surroundings. For the Otto cycle to be reversible, it would have to violate the second law.
 
siddharth23 said:
The second law of thermodynamics states that the entropy of the universe continuously goes on increasing. Even though the system may arrive at the same state after every cycle, the heat dissipated to the surroundings during the isochoric expansion increases the entropy of the surroundings. For the Otto cycle to be reversible, it would have to violate the second law.

What if we keep on replacing different temperature reservoir from time to time? If Otto cycle is irreversible, we cannot even draw it on the P-V diagram because the isochoric pressure increase/decrease are not quasi-equilibrium process.
 
Why not? Sure we can draw it on a P-V diagram. An irreversible process is just one which permantly changes surroundings. You cannot come back to the stage that was prevalent before the cycle took place.
 
kelvin490 said:
Is Carnot engine the only form of reversible engine? Is it possible to have a different form of reversible engine that goes through different processes?

For a standard Otto cycle working with ideal gas, theoretically the two processes involving isochoric pressure change can be reversible processes. Does it mean that the Otto cycle can also have same efficiency as Carnot cycle? Since temperature of the working fluid is changing during isochoric pressure change, does it mean there are infinite number of heat reservoirs being used at different temperatures so that there is no finite temperature difference at every point of the isochoric process?
The answer to all your questions is YES. You have analyzed the situation flawlessly. Very nicely done. Of course, the combined change in entropy of the two sets of reservoirs will turn out to be zero.

Chet
 
Last edited:
  • Like
Likes   Reactions: kelvin490
Chestermiller said:
The answer to all your questions is YES. You have analyzed the situation flawlessly. Very nicely done. Of course, the combined change in entropy of the two sets of reservoirs will turn out to be zero.

Chet

Thank you. I have one further question. How to compare the efficiency between a Carnot engine and an ideal Otto engine? As mentioned before in an ideal Otto engine there are infinite number of heat reservoirs being used at different temperatures so that there is no finite temperature difference at every point of the isochoric process. Carnot cycle involves only two reservoirs so it's easy to calculate the efficiency. For an ideal Otto cycle many reservoirs involved so I wonder what's the basis of comparison?
 
kelvin490 said:
Thank you. I have one further question. How to compare the efficiency between a Carnot engine and an ideal Otto engine? As mentioned before in an ideal Otto engine there are infinite number of heat reservoirs being used at different temperatures so that there is no finite temperature difference at every point of the isochoric process. Carnot cycle involves only two reservoirs so it's easy to calculate the efficiency. For an ideal Otto cycle many reservoirs involved so I wonder what's the basis of comparison?
Excellent questions. For the Otto cycle, you can of course model it yourself to derive an equation for the efficiency, or you can check out this link: http://en.wikipedia.org/wiki/Otto_cycle. In this link, they do the analysis for you. If it were me and I really wanted to get some practice, I would model it myself; otherwise, I would just see what they do in the link.

Chet
 
  • Like
Likes   Reactions: kelvin490
kelvin490 said:
Thank you. I have one further question. How to compare the efficiency between a Carnot engine and an ideal Otto engine? As mentioned before in an ideal Otto engine there are infinite number of heat reservoirs being used at different temperatures so that there is no finite temperature difference at every point of the isochoric process. Carnot cycle involves only two reservoirs so it's easy to calculate the efficiency. For an ideal Otto cycle many reservoirs involved so I wonder what's the basis of comparison?


For calculating the efficiency of an Otto cycle, use the basic principle of efficiency. How much was the heat input, how much of it was converted to work and how much heat was wasted. You can get an equation in the form of 'T'.
 
  • Like
Likes   Reactions: kelvin490
siddharth23 said:
For calculating the efficiency of an Otto cycle, use the basic principle of efficiency. How much was the heat input, how much of it was converted to work and how much heat was wasted. You can get an equation in the form of 'T'.

Agree. But I think we can only get the equation in terms of ratio of T instead of the exact temperature, since there are numbers of reservoirs and we don't have the criteria for selecting one of them as a representative heat reservoir. Is that correct?
 
  • #10
kelvin490 said:
Agree. But I think we can only get the equation in terms of ratio of T instead of the exact temperature, since there are numbers of reservoirs and we don't have the criteria for selecting one of them as a representative heat reservoir. Is that correct?
What do they end up with in the Wiki article?
 
  • Like
Likes   Reactions: kelvin490
  • #11
kelvin490 said:
Agree. But I think we can only get the equation in terms of ratio of T instead of the exact temperature, since there are numbers of reservoirs and we don't have the criteria for selecting one of them as a representative heat reservoir. Is that correct?

You're right. You get it as a ratio of temperatures. But The ratio is of temperatures at the start and end of a process. The infinite number of temperature reservoirs is a concept used to explain the process. Don't be stuck on that.
 
  • Like
Likes   Reactions: kelvin490
  • #12
Chestermiller said:
What do they end up with in the Wiki article?

Oh, yes. They express it in terms of changes in internal energy first and express in terms of initial and final temperatures. Thanks a lot.
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 8 ·
Replies
8
Views
15K
Replies
12
Views
3K
  • · Replies 19 ·
Replies
19
Views
5K
Replies
8
Views
3K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 33 ·
2
Replies
33
Views
5K
  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 1 ·
Replies
1
Views
2K