Phase change in heat engines & heat pumps

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Discussion Overview

The discussion revolves around the desirability of phase changes between liquid and vapor in the context of heat engines and heat pumps. Participants explore how these phase changes affect the work output and efficiency of thermodynamic cycles, particularly through the analysis of P-V diagrams.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that a larger area enclosed by the loop in a P-V diagram is desirable for heat engines but undesirable for heat pumps, suggesting that phase changes may influence this area.
  • Others argue that for heat engines, increasing the area vertically is preferable, while for heat pumps, horizontal expansion is more beneficial, indicating that maximizing area is not necessarily the goal.
  • A participant questions the necessity of phase changes, noting that the Carnot Cycle can enclose a non-zero area without them, prompting a discussion on practical implementations.
  • Some contributions highlight that phase changes facilitate heat absorption and rejection at different temperatures, which is crucial for the operation of heat pumps.
  • One participant mentions their self-study of thermodynamics and the challenges of visualizing processes using T-s and P-v diagrams, suggesting that both types of diagrams have their advantages and limitations.

Areas of Agreement / Disagreement

Participants express differing views on the implications of phase changes for heat engines and heat pumps, with no clear consensus on whether these changes are more desirable for one application over the other. The discussion remains unresolved regarding the overall impact of phase changes on efficiency and work output.

Contextual Notes

Participants note limitations in their understanding of the practical applications of ideal gas cycles versus those involving phase changes, as well as the challenges in visualizing thermodynamic processes through different types of diagrams.

Redbelly98
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This question has been in the back of my mind for a while. In short, is having a phase change between liquid and vapor more desirable for a heat engine or for a heat pump?

Clearly, having a large area enclosed by the loop in a P-V diagram increased the amount of work in the cycle, so anything that enlargens that area would be desirable for a heat engine and undesirable for a heat pump or refrigerator. So, does a liquid-vapor phase change within the cycle tend to increase or decrease this area -- or is there no general answer?
 
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Redbelly98 said:
Clearly, having a large area enclosed by the loop in a P-V diagram increased the amount of work in the cycle, so anything that enlargens that area would be desirable for a heat engine and undesirable for a heat pump or refrigerator.
No, I don't think so. I've never really thought about it in those terms, but it seems to me that for a heat engine you want to increase the area vertically and for a heat pump you want to increase it horizontally, but an overall enlarging is not necessarily desirable: efficiency is about the ratio between work and heat, not about maximizing the work or heat for a given mass flow rate.
So, does a liquid-vapor phase change within the cycle tend to increase or decrease this area -- or is there no general answer?
Well, without a liquid-vapor change, the area inside would be zero. The change in state is what enables the horizontal stretching because that's where the input and output of heat happens. The magic of a heat pump is in having the phase changes happen at two different temperatures, allowing heat absorption from an area that's already cold and heat rejection to an area that's already warm.
 
russ_watters said:
No, I don't think so. I've never really thought about it in those terms, but it seems to me that for a heat engine you want to increase the area vertically and for a heat pump you want to increase it horizontally, but an overall enlarging is not necessarily desirable: efficiency is about the ratio between work and heat, not about maximizing the work or heat for a given mass flow rate.
Okay, that does sound like a better way of thinking about it. Thanks.

Well, without a liquid-vapor change, the area inside would be zero.
I think I'm missing something. The Carnot Cycle (for example) for an ideal gas would enclose a non-zero area, without a phase change. Or is it a matter of what is practical to actually build and operate?

The change in state is what enables the horizontal stretching because that's where the input and output of heat happens. The magic of a heat pump is in having the phase changes happen at two different temperatures, allowing heat absorption from an area that's already cold and heat rejection to an area that's already warm.

BTW, I've started doing some self study with a copy of Cengel & Boles's Thermodynamis (3rd ed.) The chapter on refrigerators and heat pumps is full of T-s diagrams, no P-v ones which would help me visualize the process better. When I can, I'll try constructing P-v diagrams for water as well as refrigerant from the tables in the book.
 
Last edited:
Redbelly98 said:
I think I'm missing something. The Carnot Cycle (for example) for an ideal gas would enclose a non-zero area, without a phase change. Or is it a matter of what is practical to actually build and operate?
Hmm... you're right, but I'm trying to envision whether an ideal-gas heat pump could actually be built...

...I suppose you could: when you compress air with an air compressor, it heats up. When you expand it through a throttling valve, it cools. Then I guess maybe the real reason we don't use them is that the heat energy of the compression is a lot smaller than the pressure energy, so the efficiency would be pretty low. There is a lot of energy involved in a phase change - I suppose that widens the diagram.
 
Redbelly98 said:
BTW, I've started doing some self study with a copy of Cengel & Boles's Thermodynamis (3rd ed.) The chapter on refrigerators and heat pumps is full of T-s diagrams, no P-v ones which would help me visualize the process better. When I can, I'll try constructing P-v diagrams for water as well as refrigerant from the tables in the book.

Often times it's convenient to show both T-s and P-v diagrams for a cycle. A P-v diagram has trouble showing a isentropic process while a T-s diagram has difficulties showing an isobaric process.

For example, if you wiki the Brayton cycle (what gas turbine engines are typically modeled as), it shows both
http://upload.wikimedia.org/wikipedia/commons/3/3c/Brayton_cycle.svg

It just so happens to be more convenient in the refrigeration cycle to show it in the T-s diagram because it's easier to visualize the phase change...IMHO.
 

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