DaleSpam said:
Each of these definitions are used in their respective theories, and nothing in the quotes demonstrates the self-inconsistency you are claiming.
Thank you for your opinion.
DaleSpam said:
As I have mentioned, I think this is what the Feynman and French quotes refer to, not your claim that energy defies definition.
And thus we are going to end up simply disagreeing. It’s not as if Feynman is here to clarify..
DaleSpam said:
Among others. Definitions that I can think of are "capacity to do work", "Noether current for time symmetry", "the energy operator", "time time component of stress energy tensor", "KE and anything that can be converted to KE", "ADM energy", "Komar energy", etc. For your position to be correct you need to show that each is a self-contradictory definition.
I disagree with all those. I don’t think it’s worth going on about it though. I think we both understand what the other’s view is at this point and when that happens its no use continuing.
DaleSpam said:
I was not talking about the Jacobi integral. I was talking about Noether's theorem, which is more general.
Consider the example of a discreet system. In such case Noether’s theorem refers to the fact that when the Lagrangian is independent of time that Jacobi’s integral is an integral of motion. However it’s a well known fact that Jacobi’s integral is not necessarily the total energy of the system. There are specific conditions which the system must meet in order for Jacobi’s integral to be the energy. It’s quite possible for h to be constant but not the energy. This is stated quite clearly in the following places
Classical Mechanics – Third Edition, Goldstein, Safko and Poole, page 345
Classical Dynamics, Donald T. Greenwood, pages 73 and 167
Analytical Mechanics – Fifth Edition, Fowles and Cassidy, page 368
Analytical Mechanics with an Introduction to Dynamical Systems, Josef S. Torok page 124
Greenwood’s text uses the term
Natural System to refer to those systems where the value of Jacobi’s integral is the total mechanical energy.
The theorem is proven based on the
definition of
mechanical energy being the sum of the total kinetic energy T and the sum of the total potential energy V. I.e. the proof of the theorem starts out by
defining T and
defining V and
defining E as E = T + V and then
proving that E = constant for a natural system. For continuous systems something similar holds. I.e. one
defines the time-time component of the stress-energy-momentum tensor to be energy,
not by defining energy to be the the time-time component of the stress-energy-momentum tensor.
DaleSpam said:
You have this exactly backwards.
What I said is precisely correct. Simply turn to Goldstein et al and turn to section 2.7 page 62 and follow the derivation. You’ll see that for a natural system the authors state “…, so that h = T + V + E, and the energy function is indeed the total energy.”
DaleSpam said:
If you have a definition for energy then whatever meets that definition IS energy, by definition. If h is defined as energy then the point of the equality h=T+V is to show that T+V is energy.
I, like Feynman and French, have stated numerous times above that there is a
well defined definition of total
mechanical energy for discrete systems and
electromagnetic energy for electromagnetic systems etc. The
forms of energy are very well defined. It’s the definition of energy itself that defines definition.
Please recall where I quoted
Newtonian Mechanics by A.P. French, The MIT Introductory Physics Series. From page 376-368
The above remarks do not really define energy. No matter. It is worth recalling once more the opinion that H.A. Kramers expressed: "The most important thin and most fruitful concepts are those to which it is impossible to attach a well-defined meaning." The clue to the immense value of energy as a concept lies in its transformation. It is conserved - that is the point. Although we may not be able to define energy in general, that does not mean that is only a vague, qualitative idea.
Just so that we’re clear I’m going to post another expression of my position as given in
An Introduction to Thermal Physics by Daniel V. Schroeder, page 17
To further clarify matters, I really should give you a precise definition of energy. Unfortunately, I can’t do this. Energy is the most fundamental dynamical concept in all of physics, and for this reason, I can’t tell you what it is in terms of something more fundamental. I can, however, list the various forms of energy – kinetic, electrostatic, gravitational, chemical, nuclear – and the statement that, while energy can often be converted from one form to another, the total amount of the energy in the universe never changes.
The author has a PDF file online about this entitled
What is Energy at
http://physics.weber.edu/schroeder/eee/chapter1.pdf
Again the author writes
What is energy, in the scientific sense? I’m afraid I don’t really know. I sometimes visualize it as a substance, perhaps a fluid, that permeates all objects, endowing baseballs with their speed, corn flakes with their calories, and nuclear bombs with their megatons. But you can’t actually see the energy itself, or smell it or sense it in any direct way—all you can perceive are its effects. So perhaps energy is a fiction, a concept that we invent, because it turns out to be so useful.
One example of a failed definition of energy is
The ability to do work. One might mistake that for being momentum. After all, anything that has momentum can do work since changes in momentum means there is a force and that force can do work. But that's tricky stuff. E.g. suppose that during the time period t1 to t2 a block is being pushed across a table at constant speed. The total work done is zero since there is no change in kinetic energy. The force pushing it is opposed by friction so that it doesn't accelerate. Each force cancels since the mome ntum of the block doesn't change.
So again, I hold this to be quite true. Nothing that has been posted up to this point has there been any definition that would include things like zero point energy or the energy in the universe when it reaches its eventual heat death.
For some reason I failed to get across that certain forms of energy are well defined and that’s the forms of energy that Noether’s theorem is able to address. At least the proofs that I’ve seen to date.
By the way; my position is not rooted in a lack of trying to find a suitable definition. I’ve searched extensively everywhere that I have access to in order to find a definition which I hold to be correct but never found one.
Just to save you a lot of trouble I'll state that I understand that you’ll disagree with my position even given what I’ve posted just now. After all, no sense of wasting a time when I pretty much understand your position. I just disagree with it. And not because I think it's a matter of opinion, but because I haven't seen a proper definition to date including what you've posted in this thread.
Now I'm not sure if I made the mistake of saying that it
can't be defined. Only that
today I know of no logically acceptable definition of it. At least in my opinion.
To really understand what Feynman meant in that quote you
must read that section? It's in Volume 1 page 4-1 to 4-2. Otherwise you'll get the wrong idea from just looking at that quote. That's why I think you're misinterpreting that quote.
Thanks for the engaging converson DaleSpam. :)