Why doesn't Q=0 instead of Q=W if T=constant in first law?

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Discussion Overview

The discussion revolves around the first law of thermodynamics, specifically the relationship between heat transfer (Q), work done (W), and internal energy (ΔU) during isothermal processes. Participants explore the implications of constant temperature on energy transfer and the nature of heat in thermodynamic systems.

Discussion Character

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

Main Points Raised

  • Some participants assert that heat (Q) is energy transferred due to temperature differences, questioning how Q can exist without a temperature change in isothermal processes.
  • Others explain that during isothermal expansion, heat energy can be entirely converted into work (W), leaving internal energy (and thus temperature) unchanged.
  • A few participants challenge the definitions of heat and internal energy, suggesting that heat can exist without being transferred and that temperature is a measure of average kinetic energy.
  • There is a discussion about the correct formulation of the first law of thermodynamics, with conflicting equations presented (Q=W-ΔU vs. Q=W+ΔU).
  • One participant seeks clarification on how isothermal conditions are maintained during expansion, questioning whether it is due to external control or the nature of energy transfer.
  • Another participant notes that isothermal expansion does not imply uniform temperature throughout the gas, emphasizing the role of a temperature reservoir in maintaining constant temperature at the gas's surface.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and implications of heat transfer, the nature of energy conversion during isothermal processes, and the correct formulation of the first law of thermodynamics. No consensus is reached on these points.

Contextual Notes

Participants highlight the complexity of thermodynamic definitions and the conditions under which energy transfers occur, indicating that assumptions about temperature and energy flow may vary based on specific scenarios.

Henrybar
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My understanding of heat is the energy transferred as a result of temperature imbalance between systems.
If two systems at different temperatures are in contact with each other, a temperature change for both systems and an energy transfer Q is occurring.

It is known that Q=W for a closed system when T=constant according to the first law of themo, but how can there be heat (energy transfer as a result of temperature imbalance between systems) and yet no change in temperature of the system?
 
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When we have two bodies A and B and flow of heat Q say from A to B (that means that B is in lower temperature than A) then normally what happens is that this heat energy goes as whole as an increase in the internal energy of body B hence it increases its temperature and eventually (after some flow of heat for some time ##\Delta t## ) the temperature of B becomes equal to temperature of A.
However what happens during say an isothermal expansion of a gas, the energy heat Q that flows to the gas does not go to increase its internal energy, rather it goes as whole to do mechanical work W. So its not the internal energy (and hence not the temperature ) that increases, it is rather the work done by the system that increases. In other words all the heat energy that flows into the gas, is being transformed into mechanical work W, and nothing at all goes to internal energy of the gas, hence its temperature stays constant.
To state it again in a final simplified way:
When all or part of heat energy Q is being transformed to internal energy then the temperature increases.
BUT when all heat energy Q is being transformed to mechanical work, then it is the mechanical work W done by the gas that increases, while its internal energy and temperature remain constant.
 
Henrybar said:
My understanding of heat is the energy transferred as a result of temperature imbalance between systems.
If two systems at different temperatures are in contact with each other, a temperature change for both systems and an energy transfer Q is occurring.

It is known that Q=W for a closed system when T=constant according to the first law of themo, but how can there be heat (energy transfer as a result of temperature imbalance between systems) and yet no change in temperature of the system?
Are you familiar with the first law of thermodynamics. If so, please write it out for us in equation form.
 
Henrybar said:
My understanding of heat is the energy transferred as a result of temperature imbalance between systems.
This is wrong. Heat is energy, whether it is transferred or not. It can be transferred, but that is not necessary. (I have been corrected on this.)
If two systems at different temperatures are in contact with each other, a temperature change for both systems and an energy transfer Q is occurring.

It is known that Q=W for a closed system when T=constant according to the first law of themo, but how can there be heat (energy transfer as a result of temperature imbalance between systems) and yet no change in temperature of the system?
If you are talking about the transfer of heat within one isolated system, rather than the transfer of heat from one system to another, then you can have Q=W=0.
 
Last edited:
FactChecker said:
This is wrong. Heat is energy, whether it is transferred or not. It can be transferred, but that is not necessary.
In thermodynamics, heat is defined as energy in transit across the boundary of a system as the result of a temperature gradient at the boundary, or as a result of a temperature difference between the system and its surroundings.
 
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Chestermiller said:
In thermodynamics, heat is defined as energy in transit across the boundary of a system as the result of a temperature gradient at the boundary, or as a result of a temperature difference between the system and its surroundings.
Ok. I stand corrected (and surprised)
 
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FactChecker said:
Ok. I stand corrected (and surprised)
I should not have been surprised since temperature is used to measure the average kinetic energy of the particles in the system. Heat is something else.
 
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Chestermiller said:
Are you familiar with the first law of thermodynamics. If so, please write it out for us in equation form.
Q=W-ΔU
Heat added to system=work done by system - change in internal energy of system
 
Henrybar said:
Q=W-ΔU
Heat added to system=work done by system - change in internal energy of system
Wrong. Try again.
 
  • #10
Delta² said:
When we have two bodies A and B and flow of heat Q say from A to B (that means that B is in lower temperature than A) then normally what happens is that this heat energy goes as whole as an increase in the internal energy of body B hence it increases its temperature and eventually (after some flow of heat for some time ##\Delta t## ) the temperature of B becomes equal to temperature of A.
However what happens during say an isothermal expansion of a gas, the energy heat Q that flows to the gas does not go to increase its internal energy, rather it goes as whole to do mechanical work W. So its not the internal energy (and hence not the temperature ) that increases, it is rather the work done by the system that increases. In other words all the heat energy that flows into the gas, is being transformed into mechanical work W, and nothing at all goes to internal energy of the gas, hence its temperature stays constant.
To state it again in a final simplified way:
When all or part of heat energy Q is being transformed to internal energy then the temperature increases.
BUT when all heat energy Q is being transformed to mechanical work, then it is the mechanical work W done by the gas that increases, while its internal energy and temperature remain constant.

I should have mentioned my question does particularly concern the isothermal expansion of gas. I have a few things I would like final clarification on.
How is an isothermal expansion of a gas maintained if there is a temperature imbalance (and heat transfer)? Is it because the experimenter is not allowing the temperature to change? Or is because the energy simply goes into work only, but why would it only go to work?
 
  • #11
Chestermiller said:
Wrong. Try again.
Q=W+ΔU
Heat added to system=work done by system + change in internal energy of system
 
  • #12
Isothermal expansion does not mean that the temperature of the gas is constant throughout its volume during the entire expansion. It means that the gas is kept in contact with a constant temperature reservoir that is held at the original temperature of the gas as the gas expands. As the gas expands, its interior cools (temporarily) as a result of the work it does, and heat then begins to flow between the constant temperature reservoir and the gas. When the gas approaches its final thermodynamic equilibrium state, it again equilibrates with the temperature of the reservoir. So, in an "isothermal expansion," only the surface of the gas in contact with the reservoir is at constant temperature throughout the process. The rest of the gas experiences lower temperatures (until the end).
 

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