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Alternative definitions of energy?

 
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Dec9-11, 06:02 AM   #137
 

Alternative definitions of energy?


Quote by kith View Post
No. In my example, the entropy of the open system always increases. If you think otherwise, please tell me where exactly you disagree with it.
I already said you that tracing is a time-reversible operation. If you start from a reversible equation and apply the trace over environmental degrees of freedom, the resulting equation for the open system is time reversible and violates the second law.

Of course, if you apply some of the «mathematical funambulism» so popular in a part of the so-called open systems quantum literature, then you can prove anything that you want...

For this reason, the Brussels school (and others serious guys) now{*} start from an irreversible equation for the isolated system (a generalization of QM) and then obtain the correct irreversible equation for the open subsystem.

I am so tired of the plain nonsense written in part of the literature on irreversibility that I plan to write a paper probably titled «mathematical funambulism on the theories of irreversibility» or something as that. But not now. Now I am with a paper that generalizes the first and second law of thermodynamics to open systems (yes also in this topic many literature in open systems is wrong).

Quote by kith View Post
The situations are different. In both cases, we have a system with an exact equation and an approximate equation. In the relativity case, the exact equation predicts all observed facts. Now let's take your viewpoint for the irreversibility case. Then, we have an observed fact (irreversibility), which is not predicted by the exact equation, but only by the approximate one. Now you argue, that the approximate equation can be used to explain this observed fact. But simultaneously, you seem to think that the exact description is given by the "exact" equation. This doesn't make sense to me.

I don't say that the TDL doesn't give the right answers for finite systems. I just say, it can't be used in explaining them.
If you read the authors' work you will discover that they are not saying that the irreversible equation is inexact. At contrary they claim that it is the reversible equation which is inexact.

There are several subtle technical issues in the meaning of the TDL in their work that you fail to understand, this limit is not being taken to approximate the equation from other. It is being taken to eliminate some spurious non-Markovian effects related to the evolution of correlations in the multiparticle system (which does not follow the Liouville equation).

The reason which they take this limit is also related to the fact that the exact mathematical nature of the extended space is not still well-understood, and neither them nor any mathematician knows how to obtain the specific spectral decomposition in a pure ab initio fashion. Although in the same volume in Adv. Chem. Phys. a mathematician claims to obtain the spectral decomposition using a new algebra, without appealing to the TDL anymore.

In my own view (sometimes discussed with relevant member of the Brussels school including the Nobel laureate himself) the resulting irreversible equation is the result of bifurcation points in the extended Liouville space, but for LPSs the non-Markovian terms are lost and the irreversibility generated by those points mimics what would obtain from a fictitious TDL.

That is, the TDL is a simple way to introduce the elements lost by the Markovinization. It is a kind of trick to obtain some results, althought you pretend to take it seriously even after being warned to not do it.

This is not very different from starting from Newtonian p=mv and then obtaining the relativistic momentum by doing a trick m→m(v). Evidently, the analogy is not complete, specially because the math behind SR is well-understood and easy and such tricks are not more needed to obtain a relativistic momentum.

It is not very different from the TDL in equilibrium SM. This trick is used to simplify some mathematical derivations otherwise would be very difficult to do or without rigor (or both).

{*} As said they did your same mistake in the past
 
Dec9-11, 06:15 AM   #138
 
The timescale of the transfer is not universal and depends of each process. In thermodynamics of processes the first law (for closed systems) is generalized to

dU/dt = dQ/dt + dW/dt

but thermodynamics alone cannot say you the rates. The rates are obtained from rate equations as Fourier law, chemical kinetics laws, diffusion laws, etc.

If A and B are contiguous then energy either belong to A or to B. If the systems are not contiguous, then energy could be stored in some intermediate system C before arriving at B.
Whilst I am grateful for your reply, I am disapointed with the level of the response, considering the high level of your other posts.

You have in another post commented upon mathematical exactitude, but offer the highly restricted formulae for the First Law since the integration of both dQ and dW is, in general, path dependent.

Secondly none of the time dependent processes you mention apply to my comment. They all apply to energy transport within a system and fail at the interface between systems, which is what I am talking about.

What I am referring to is another facet of the 'action at a distance' problem, which I am sure you are familiar with. This goes much deeper than schoolboy thermodynamics.
 
Dec10-11, 07:03 AM   #139
 
Quote by Studiot View Post
Whilst I am grateful for your reply, I am disapointed with the level of the response, considering the high level of your other posts.

You have in another post commented upon mathematical exactitude, but offer the highly restricted formulae for the First Law since the integration of both dQ and dW is, in general, path dependent.

Secondly none of the time dependent processes you mention apply to my comment. They all apply to energy transport within a system and fail at the interface between systems, which is what I am talking about.

What I am referring to is another facet of the 'action at a distance' problem, which I am sure you are familiar with. This goes much deeper than schoolboy thermodynamics.
Then it seems evident that I did not understand your questions. Unfortunately I do not understand them now either.

I do not understand what is the link between what you say about dQ and dW and what I wrote dQ/dt and dW/dt

I do not understand why you say that the time dependent processes I mentioned apply to energy transport within a system and fail at the interface between systems when

dU/dt = deU/dt = dQ/dt + dW/dt

the subscript «e» meaning «external». I.e., the above expression gives the changes in internal energy due to flows through the boundary surface that encloses the system volume. The above expression does not apply to energy transports inside the system. The corresponding expression for changes in the energy due to internal processes is

diU/dt = 0

which is another way to state conservation of energy.

And, finally, I miserable fail to understand what do you mean by «another facet of the 'action at a distance' problem»
 
Dec11-11, 01:55 PM   #140
 
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Quote by Studiot View Post
Whilst I am grateful for your reply, I am disapointed with the level of the response, considering the high level of your other posts.

You have in another post commented upon mathematical exactitude, but offer the highly restricted formulae for the First Law since the integration of both dQ and dW is, in general, path dependent.

Secondly none of the time dependent processes you mention apply to my comment. They all apply to energy transport within a system and fail at the interface between systems, which is what I am talking about.

What I am referring to is another facet of the 'action at a distance' problem, which I am sure you are familiar with. This goes much deeper than schoolboy thermodynamics.
Studiot, thanks for making reference to 'action at a distance', searching wiki has opened a vast number of related links that have helped me understand much more, in many areas.

Like Juanrga, I do not know your meaning of "fail at the interface between systems". To me this is a boundry for mass, but not thermal energy. If by design, this interface can represent a storage of, and a speed control for energy moving between systems A and B. As mentioned before, any number of sub-systems within a design.

Again, thanks. I am learning a lot from this thread.
 
Dec21-11, 11:35 AM   #141
 
Unfortunately I do not understand them now either.
Here is a quote from Maxwell that nicely sums up my question.

we are unable to conceive of propagation in time, except either as the flight of a material substance through space, or as the propagation of a condition of motion or stress in a medium already existing in space... If something is transmitted from one particle to another at a distance, what is its condition after it has left the one particle and before it has reached the other?
 
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