Contradiction in laws of thermodynamics

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Discussion Overview

The discussion revolves around the laws of thermodynamics, particularly the first and second laws, and their implications regarding energy, work, and entropy. Participants explore concepts related to energy transformation, the availability of energy for work, and the nature of entropy in thermodynamic systems.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant states that energy is the ability to do work and questions whether work consumes energy, suggesting a misunderstanding of energy conservation.
  • Another participant clarifies that energy does not cease to exist when consumed in work but transforms from one form to another.
  • It is proposed that when entropy reaches its maximum, no usable energy remains, although energy is still conserved in a form that cannot be utilized.
  • A participant emphasizes that energy is only available for work when there is a temperature difference, and at equilibrium, the kinetic energy of molecules is uniform, limiting energy conversion to mechanical work.
  • Some participants challenge the definition of energy as merely the ability to do work, suggesting it is overly simplistic and may hinder understanding.
  • There is a discussion about the mean kinetic energy in equilibrium systems and the distribution of particle velocities, with a call for careful language in describing these concepts.

Areas of Agreement / Disagreement

Participants express differing views on the definition of energy and its implications for understanding thermodynamic processes. There is no consensus on whether the traditional definition of energy is adequate or if it should be revised. Additionally, the interpretation of entropy and its relationship to usable energy remains contested.

Contextual Notes

Participants note the importance of definitions and the potential for misunderstanding when discussing energy and work. The discussion highlights the complexity of thermodynamic concepts and the need for precision in language.

apurvmj
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following is what little I know about energy:Energy: its the ability to do the work.

First law says you cannot create nor destroy energy but can transform it to from one form to another. so its always 100 % conversation. but in a process you have 'work' done also. so does that mean 'work' doesn't consume energy.

In second law; entropy always increase but cannot decrease. In other words system always tends to achieve thermal equilibrium. Does it mean at its peak you left no usable energy, why? when you have 100 % conversation or has energy got destroyed.

Thanks for your explanations (in advance)
 
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If by "consume" you mean the energy ceases to exist, no.

For entropy, yes, it means temperature equilibrium.
 
* Work is energy flowing from one form to another. If for instance you push an object and it accelerates, its kinetic energy is increases because work has been done on it by the force that made it accelerate. But that energy must have come from elesewhere (The chemical energy in your mussels, for instance) so the total energy has not changed.

* Yes when entropy reaches its maximun, no usable energy is left. Energy is still conserved but it is in a format that canot be used any more.

Both your questions seem to be related to the stupid definition for energy given in introductory textbooks "Energy is the ability to do work". Dump that definition and you will be one step closer to understanding.
 
Energy is only 'available' to do work (a heat engine, for example) when there is a temperature difference. At equilibrium, with an ideal gas and a simple model, the Kinetic Energy of the molecules (temperature) is the same, everywhere so there is none available for conversion to mechanical energy (to do work).
I would not use the word "peak" in your original question. It's more of a limiting, maximum situation and will not decrease again.
 
dauto said:
* Yes when entropy reaches its maximun, no usable energy is left. Energy is still conserved but it is in a format that canot be used any more.
Entropy does not reach an absolute maximum. The ability to use internal (thermal) energy (ie the ability to use thermal energy to produce mechanical work) just requires a temperature difference.

Both your questions seem to be related to the stupid definition for energy given in introductory textbooks "Energy is the ability to do work". Dump that definition and you will be one step closer to understanding.
There is no need to change the definition of energy. Energy is the ability to do work. Work is the application of a force through a distance. Increasing the speed of a molecule requires work being done on that molecule. So it takes work to randomly increase the kinetic energy of molecules to increase temperature. This may not result in useful mechanical work on a macroscopic scale, but it still represents work being done at the microscopic level.

AM
 
sophiecentaur said:
At equilibrium, with an ideal gas and a simple model, the Kinetic Energy of the molecules (temperature) is the same

The mean kinetic energy uniform throughout the system in equilibrium, but the velocities of the particles will still be characterized by a distribution function.

Your argument remains the same, but I think it's worth being careful about these things.
 
Last edited:
ZombieFeynman said:
The mean kinetic energy uniform throughout the system in equilibrium, but the velocities of the particles will still be characterized by a distribution function.

Your argument remains the same, but I think it's worth being careful about these things.

Agreed. I should have included the word 'mean' in there.
 

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