ZapperZ said:
1. You brought up the "hydrodynamical equations"
2. *I* said that "hydrodynamical equations" in superconductivity is something like the London equations. What else is there? You didn't say that. *I* did.
3. I then said that this hydrodynamical equations represented by London equations are not fundamental.
4. That is why I wanted you to explain where such a thing comes in, because it CAN'T be just "hydrodynamical", because these can easily be phenomenological. I asked this way in the beginning when I responded to your post. I asked this repeatedly. To say that something is "hydrodynamical" in superconductivity means it isn't fundamental, because it isn't the starting point!
I didn't! Read above! I was the one who wanted you to explain how it actually can derive superconductivity. I believe Reilly also asked you the same thing.
Notice that I was not the one who claim that all of condensed matter physics based based on such "hydrodynamical" equations. My first question to you want to seek such clarification. It never came, even till now. And it is strange how one can look at "section" on superconductivity in Tinkham and not look at BCS section. All you did was look at the phenomenological models then, which are not fundamental.
BCS doesn't derive Madelung equations. BCS doesn't even USE such a thing (did you find any reference to Madelung equation in Tinkham at all? What about in Mahan?). So as I asked in the very first question, where did this come in many-body physics and superconductivity? In other words, we are back to the very first square.
I'm done!
Zz.
I'm done!
That's fine. Then you won't mind if I give the last words.
2. *I* said that "hydrodynamical equations" in superconductivity is something like the London equations. What else is there? You didn't say that. *I* did.
Thank you, I'm happy you corrected yourself. But actually, you said the hydrodynamical equations "ARE" the London equations, not just that they are "something like" the London equations. I could easily quote you. You seemed to entirely miss the fact that I have ALWAYS been talking about the the Madelung equations, when I say "hydrodynamical". So HYDRODYNAMICAL = MADELUNG EQUATIONS, AND MADELUNG EQUATIONS = NONLINEAR SCHROEDINGER (GROSS-PITAEVSKI) EQUATIONS.
3. I then said that this hydrodynamical equations represented by London equations are not fundamental.
So hopefully you see now that this was not what I was asking about. I was talking about the Madelung equations.
That is why I wanted you to explain where such a thing comes in, because it CAN'T be just "hydrodynamical", because these can easily be phenomenological. I asked this way in the beginning when I responded to your post. I asked this repeatedly.
But then I said I was NEVER claiming these Madelung equations were "fundamental" in the sense of BCS theory. And you then said you could derive these hydrodynamical equations from first principles, and therefore that if these are the equations of BQM, then the equations of BQM cannot be fundamental. So I then asked you to justify how you could derive the Madelung equations (and therefore the nonlinear Schroedinger equation they are equivalent to). Now maybe you were referrring to the London equations, but then that means you weren't listening to me carefully in the beginning, as I was ALWAYS talking about the Madelung equations as the hydrodynamical equations, and the equations of BQM.
I believe Reilly also asked you the same thing.
Actually he did not. He asked me 4 entirely different questions, which I addressed, and he eventually conceded in private.
Notice that I was not the one who claim that all of condensed matter physics based based on such "hydrodynamical" equations. My first question to you want to seek such clarification. It never came, even till now.
Actually that clarification did come. In case you forgot, let me quote myself from the electrons thread:
No, the way you quote me brought it out of context. It sounds like I'm saying all of condensed matter owes its success to the equations of BQM, which is not what I said. I said it owes much of its practical and methodological success to the equations of QM. But I should have been more specific, namely, the theory of superconductiivyt and superfluidity owes much of its practical success to the equations of BQM. And indeed that is definitely true as Feynman, Likharev, Visser et al., show.
All you did was look at the phenomenological models then, which are not fundamental.
Yes, because I wanted to hear from you first how the Madelung and Schroedinger equations, which are according to you phenomenological, could be derived from first principles.
BCS doesn't derive Madelung equations. BCS doesn't even USE such a thing (did you find any reference to Madelung equation in Tinkham at all? What about in Mahan?).
OK, if BCS doesn't derive or use the Madelung equations, then what you said earlier about the equations of BQM not being fundamental, is not true. I referenced in the electrons thread the section in Tinkham's book to look at. I was the superconductivity and superfluidity chapter (I forget which chapter number).
So as I asked in the very first question, where did this come in many-body physics and superconductivity? In other words, we are back to the very first square.
I'll quote Feynman once again:
"Schroedinger's equation for the electron pairs in a superconductor gives us the equations of motion of an electrically charged ideal fluid. Superconductivity is the same as the problem of the hydrodynamics of a charged liquid.
If you want to solve any problem about superconductors you take these equations for the fluid adn combine them with the Maxwell equations to get the fields" p. 21-13/14.
This applies, by the way, for N particles.
Cheers,
Maaneli