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Superconductivity at room temperature??

Furthermore I told you that you are ignoring boundary conditions. To do the calculation one should know how the charges are attached to the disc. Have you, for example, used an acrylic polymer? Then the charges form part of a dielectric: Only a complete idiot will solve Maxwell's equations without taking this into account.

You are wrong. The solution ignoring the disk-material is perfectly reasonable and does not radiate. The solution taking into account the disk-material is also reasonable, but also does not radiate. The solution taking into account the disk material, Special Relativity, and the slight paramagnetism of oxygen in the air near the disk? Sorry, that still doesn't radiate.

You are on a fishing expedition. We have presented a clear and simple example of accelerating charges that according to Maxwell do not radiate. You are fishing for details that you hope might prove this example wrong. Your hopes are unfounded.

This charade that your fishing-guesses are actually counterarguments, as opposed to guesses-that-you-hope-will-become-counterarguments, is dishonest.

Even if the acceleration and speed are perpendicular to each other the charge-carrier will radiate.

Except in the counterexamples.

They already knew this nearly 100 years ago after Rutherford claimed that electrons can circle a nucleus. They cannot do so ever without radiating EM and spiraling into the nucleus.

The orbiting point charge was not one of the counterexamples.
 
As a lurked on this thread, I'd just like to thank Ben M, Ziggurat and Sol Invictus (amongst others) for their clear explanations on this topic, especially in the face of the continuing insults coming from Johan.
 
I have been following this and it seems like somewhere along the line, there was a massive derail from the original idea of something about diamonds and vacuum being a superconductor at room temperature. Now it is just a bunch of nit picking and name calling.

I love the part where Johan accuses someone of thinking he is God, because he is an idiot and arrogant, etc. Good stuff.:D

I have dealt with dozens of profs and very well known chemists in professional situations, designing equipment for them, but I have never had anyone call me an idiot when I proposed a project or discussed an idea. I would have kicked him out if he had.:) I'm surprised no one here has reported any of this insulting behavior. Attacking the arguer by both factions. To my mind, when anyone starts this "you're an idiot" stuff or "you should leave this to the pros", it generally means he is clueless and is covering up his inadequacies.

To be fair to Johan, he has been grossly misunderstood on several occasions, and the frustration of his past then shows through. His opponents are also frustrated because they do not accept what Johan is claiming, and because they perceive that he is dodging their arguments, moving goalposts etc. It is typical on these forums for people to read and not quite understand what is being said, and then they often just come back with a knee jerk reaction. This has happened with more than one issue here on both sides... even to me, the one time I stuck my nose in just to try to help. I'd love to hear the real story about the experiments and what was observed. I think we are all capable of sorting it out for ourselves.

It is certainly an interesting thread.

I have one question, if anyone should find the time. In all my reading about this, I read something that I don't quite follow. Someone made a statement that the juncture of two superconductors is superconducting. Now, I had never thought about this, but how can this claim of superconductivity be specified if the cross sectional area and the pressure or force applied to the two superconductors is not made specific? Is this essentially the basis for the Josephson junction? In other words, what if the cross section is microns, and the pressure is extremely small?
 
In addition, even if there were no loss by polarization, the energy levels will shift by qV. Thus when a charge carrier from the high energy side moves through to the low energy side, it has to lose 2qV in energy even though its charge is only q. If it does not do so you will be violating energy conservation.
There is no "free" extra energy involved since the shift in energy is qV as it is for all the energy levels PLUS a further qV since the polarization energy has also decreased.

So in your model, when one applies a voltage V to a superconducting material, the charge carriers (charge q) get qV of energy (from the electric field potential) plus a second qV of energy from polarization? Am I correct so far?

Your model then says that if you apply said voltage to the "near" side of a Josephson junction, you get both energies (2qV) back when the charge carriers cross the junction to the "far" side. Is that correct?
 
This is the paranormal picture that is in your head that the "particle bridges" states A and B. Don't put words in my mouth or think that you are God who knows what I am thinking. You are arrogant and despicable by creating a straw man which you can then attack with nonsense arguments.

It is obvious (to me) that you have some incorrect mental picture of tunneling and/or acceleration. I don't know what that picture is, all I know is that you're drawing some wrong conclusions from it.

I thought it would be useful if I knew what your underlying mental picture was---totally standard pedagogy. So I tried to guess, inventing a plausible-sounding misconception that would cause someone to make no-acceleration statements similar to yours.

Did I guess wrong? Fine, so you're not stuck in a sequence-of-stationary-states misconception. Sorry. Now I know. Unfortunately that puts us back in the state where all we know is that you think there's no acceleration involved in tunneling.
 
You say it must, I say that the experimental evidence is compelling that this transfer, although requiring energy, does not involve "classical acceleration".

What evidence?

My guess at your reasoning is as follows. Please don't be offended if I guessed wrong.

A) system X includes tunneling but, experimentally, doesn't radiate.
B) All systems that accelerate radiate.
C) Therefore system X doesn't accelerate.

If this is the reasoning, statement B is wrong so you can't conclude C from A.

So: other than "lack of radiation", what is the experimental evidence addressing acceleration in quantum systems? Citations would be appreciated.

So synchrotron radiation does not involve acceleration of charges?

Synchrotron radiation does involve acceleration. Is this so hard?

MANY accelerating charges radiate. Synchrotron light sources are some of them. I have given several examples myself. I have said this over and over. Can you acknowledge this, please? I am tired of repeating it.

OTHER accelerating charges do not (classically) radiate. Zig and I have given examples of these also. A line charge in uniform circular motion. Current going around a bend in a wire. A linearly-accelerating charge distribution (my "rope") engineered to have time-independent E and B fields.

To reiterate:

a) Do accelerating charges ALWAYS radiate? False. This is your claim, it's wrong. Spinning disks are an explicit counterexample.
b) Do accelerating charges SOMETIMES radiate? True. Synchrotrons do, spinning disks don't.
c) Do accelerating charges NEVER radiate? False. Synchrotrons are an explicit counterexample.
 
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Thanks Sol,
However the pdf file is corrupt and does not open.
No sweat, please don't waste any more of your time on this.

It opens without problems for me. If that copy really doesn't work for you, just google the name of the paper ("Unskilled and Unaware of It: How Difficulties in Recognizing One's Own Incompetence Lead to Inflated Self-Assessments"). It's well worth reading.
 
I dip in and out of this thread as one would do with a swimming pool on a hot day. I admit that as someone who (barely) obtained a BSc in physics many years ago, I find some of the maths and concepts difficult to follow but does it boil down to:

  • Man conducts an experiment and comes up with unexpected results which seem to show room temperature superconductivity or more specifically provide evidence analogous to room temperature superconductivity (as in rabbits have big ears, my mate Dave has big ears therefore my mate Dave is a rabbit)
  • Man concludes that he has found room temperature superconductivity and devises a theory to explain it
  • Man is unable to convince the scientific community of the merits of hos theory
  • Man chooses to self publish as a way of publicising this theory
  • Some time later...........
  • .......Theory comes to the attention of an internet forum some of whose members are knowledgable in the given field (and many more of whom are groundnut-pitching members of the peanut gallery)
  • They review the paper and have the temerity to suggest that.....
  • ....perhaps there may have been a flaw in the experimentaly design and/or results results interpretation and......
  • .....that the theory presented conflicts with some pretty well established and proven rules
  • Rather than considering the experimental design and/or results interpretation, Man would rather suggest undermining the cornerstones of modern physics and undertake ad-hominem attacks

I'm still not clear why johanfprins isn't willing to reconsider but such intransigence is not helping his cause.
 
It you're looking at a potential barrier, then obviously there is.
You see this is the type of irrelevant remark that gets up my nose. What it implies in terms of the discussion so far is that you believe that a charge-carrier in a superconductor can accelerate uphill against the gradient which is responsible for generating the force. Please Ziggurat, let us try and talk concisely instead of firing off cheap shots as you have been doing all along.
That's irrelevant to our discussion. What's relevant is whether or not there's an acceleration when an electron moves in a circle. And there is.
I have never disputed this for classical movement, as modeled by Ehrenfest, who reconciled classical mechanics to dovetail smoothly with quantum mechanics without the need to invoke paranormal, metaphysical concepts like "probability amplitudes".
Quantum mechanics is not any different than classical mechanics in this respect.
Under conditions for which Ehrenfest's theorem applies, you are correct. But in a superconductor the experimental evidence is compelling that the charge-carriers are moving under conditions for which Ehrenfest's theorem does not apply. This must be so since when these charge-carriers move through a Josephson junction with a voltage-gradient, so that Ehrenfest's theorem does apply, they emit EM-radiation. When they move through the superconductor, they do not emit such radiation: This means that Ehrenfest's theorem does not apply: The earth is moving my friend no matter how much you want to waste everybody's time by raising irrelevant arguments.
Ehrenfest's theorem doesn't depend on boundary conditions. It ALWAYS applies.
Oh yes it does depend on boundary conditions! It only applies when the boundary conditions are such that a gradient in the potential energy function is present. When this is not the case, Ehrenfest's theorem need not apply. According to you it must still apply for a stationary wave. Even though it seems correct to reason semantically that it is so, you are wrong since it does not always apply under these conditions; or else we would have had that the charge-carriers within a superconductor would have radiated EM.
For an atomic electron orbital in an energy eigenstate, <x> is constant, so both its first and second time derivatives are obviously zero. Ehrenfest's theorem DOES apply, and it TELLS you that there's no acceleration for an atomic orbital eigenstate. It doesn't change position at all.
Semantics, semantics, semantics. I have claimed all along that the charge-carriers within a superconductor move without accelerating, since I am compelled as a reputable physicist (fortunately with an excellent engineering background) that I must accept the experimental facts. If they did accelerate they would emit EM just as they are doing when they accelerate through a Josephson junction when Ehrenfest's theorem does apply. Since they move through the superconductor itself without emitting EM it is incontrovertible experimental proof that they are moving without being accelerated: i.e without Ehrenfest's theorem applying.
But that's not the case for the scenario we're talking about.It absolutely does. This is standard textbook quantum mechanics. As long as what doesn't exceed a time interval dt? I don't think you even know.
The energy increase which is required to move over a barrier without acceleration cannot exceed a time interval (delta)t as limited by (delta)E(delta)t=g(hbar) where the value of g is determined by the equilibrium-energy, size and shape of the wave. For a Gaussian "zero-point" wave g=1/2. So I do know!
Absolutely wrong. Also wrong. And... wrong again.
I am not really interested in the childish game if "it is' "it is not" Please grow up!
Ehrenfest's theorem always applies.
No it does not as experimentally proved: Since if it did always apply charge-accriers moving through a superconductor would emit EM, just as they do when they move through a biased Josephson junction within which Ehrenfest's theorem does apply.
You keep inventing exceptions to standard physics and attributing it to quantum mechanics, when quantum mechanics makes no such claims.
I cannot "invent" experimentally incontrovertible results: It is the experimental results that determine physics: Or should do so: Unfortunately our "modern" physicists (like you Ben and Sol?) do not believe that experimental results must be the final arbiter. No wonder physics is is a mess!
There is no logic. There is only an unsupported assertion that quantum mechanics somehow allows you to violate laws which in fact are part of that very same quantum mechanics.
The logic on which physics must be based is that you must accept experimental results even if they do not fit the logic-dogma you want to believe in: Your attitude is setting physics back by 400 years.
As I have asked you please stop your childishness of "you did" "I did not" arguments. How old are you?
That's not really good enough. The problem is that nobody believes that your limits on your voltage measurements are small enough to show that anything even unusual is happening.
You just argued that voltage measurements cannot be used to prove superconduction. Now when it suits you, you reverse your stance. You see why it is impossible to have a rational discussion with you?

In my experiment I do not need to do such experiments, even if I could do them, since the physics that is used to model electronic interfaces, and thus chips, demands that the voltage within my phase must be exactly zero. In fact, my experiment is the first ever that proves directly that the voltage is actually zero. It is the best proof ever that a current can be flowing with zero voltage.
Because at the end of the day, the voltage isn't what you want to show gets close to zero, the resistivity is. THAT is what Onnes was actually concerned about, not voltage.
How did Onnes measure the resistivity without being concerned about voltage or an electric-field? And since zero resistivity has NEVER been defined before, or after, Onnes discovered superconduction, it will be enlightening to us all on this thread if you would be so kind to give us a definition of zero resistivity: Please indulge us.
The best way to do that is not actually through current-voltage measurements, but by inducing eddy currents and measuring their decay (or lack thereof).
Indulge us further and tell us how these eddy currents are generated? You believe it is by an electric-field and I tell you that current within a superconductor cannot be generated by an electric-field whether this field is the result of a voltage or the result of a changing magnetic field.
That gets you much lower limits on the maximum resistivity.
Semantics semantics.
So if you can't do that, if you're stuck trying to read off the voltage from a fluke multimeter, well, that won't convince anyone that you don't just have a low but normal resistance. You're making an extraordinary claim. You should not be surprised if people expect extraordinary evidence.
If people cannot understand that dipoles form in order to cancel an applied electric-field (if they have enough charges that can separate), and are too stupid to understand the elementary freshman physics which demands that the electrons between the diamond and anode, and the positive depletion layer under the diamond's surface, form an equilibrium dipole within which there is no electric-field possible; and that even under these conditions (for which it is incontestable that the applied electric field is fully cancelled and thus EXACTLY zero) a current flows; then they are not fit to do physics.
Yes, you can't (and don't have to) prove that the voltage is identically zero, but you DO need to prove that its upper bound is so low that the resistance is not ordinary.
I do not need to measure an upper bound since the electric field cannot be anything else than exactly zero. If the physics of electronic interfaces, which is used every day to design microchips and which has never failed, proves beyond ANY doubt that the electric-field must be exactly zero, and you are too daft to understand solid state electronics, then the problem is with you, not with me.
No. That is not a problem. You keep claiming it is, but your reasoning is circular.
Oh yes it is since accelerated charge carriers gain kinetic energy which, even though there is no scattering, must dissipate within the target contact: There is no such dissipation for a superconductor. If you are capable, you can prove it to yourself in any simple laboratory: However, I suppose that you do not know what the inside of a physics laboratory even looks like.
Kinetic energy is only generated if the acceleration is along the direction of motion.
But to emit EM radiation this need not be so: Acceleration perpendicular to velocity will still cause radiation to be emitted.
And so what if it gets dissipated within the "target contact"?
Do you know about energy conservation? It seems not at all. Accelerate a charge-carrier from the injection contact to then target contact and it will gain kinetic energy V=(1/2)mv^2; where V is the voltage difference. This then dissipates within the contact. Now this charge-carrier is accelerated within a resistor and is thus scattered all the time on its way to the target contact so that it deposits energy within the material: Guess what? The net energy deposited , now within the material, is still V=(1/2)mv^2. So you say that the only difference between a superconductor and a conductor is that the energy in the case of a superconductor is deposited within the target contact? Thus, the electrons moving through a vacuum diode forms a superconducting phase? Please don't be so naive.
No. You have made general claims, and when I prove that your general claims are false by showing how it fails in a time-varying situation, you claim that we're not talking about such scenarios.
You are lying in order to make a cheap shot.
When I point out that the SAME failures occur in static scenarios,
You have not proved this anywhere: I have not made any claims about time-varying currents but only about equilibrium currents. If you are unable to understand the difference between the two cases the problem lies with your inability to understand physics.
First off, Ehrenfest's theorem always applies. Secondly, if a potential gradient is zero, that doesn't mean Ehrenfest's theorem doesn't apply, that just means you stick in a zero for that term.
Another semantic cheap shot. The fact that you can argue thus, does not imply that Ehrenfest's theorem always applies for a stationary wave. Ehrenfest did not consider a zero gradient when he derived his theorem. You are using "the trivial" in an attempt to avoid talking real physics.
And third, nothing prevents a potential energy gradient from existing within a superconductor, you have simply declared this to be so.
Must you always distort everything? I have said that there is not a potential gradient caused by an applied electric-field when an equilibrium current is flowing. Can you see the difference to what you are claiming. If not, you will do science a hell-of-a-favor to get out of physics.
The junction itself, even with zero field, has a potential energy gradient. If it didn't, there wouldn't BE a barrier. So even in the absence of any external voltage, electrons passing through the junction will still be accelerated.
Where have I ever written that there are no barriers. My model specifically gives a formula, which is fully commensurate with Schroedinger's equation, of how a charge carrier can scale such a barrier with a speed v without needing any acceleration. If Ehrenfest's theorem applied, as you are hell-bent on claiming, the charge-carrier will not be able to scale such a barrier ever; and you will have an insulator; not a superconductor.
And you've also claimed that they radiate more energy than you put into the system. A point you still haven't addressed.
I have described the process not well enough initially and admitted that you could have concluded that I am claiming more radiation than the energy that is available. So you do not accept this admission? Once a man has made a mistake you are a bully who will keep on kicking him even after he admitted that he was wrong?

I have since corrected the mistake AND placed the corrected version on my website AND explained it in the simplest terms possible, AND i will keep on doing so in the hope that the penny will eventually drop; even though you have proved that you are not very competent to handle real physics. I consider it my duty to explain physics over and over again until a person can understand it; even when the person involved is slow to grasp science.

I have now spent the whole morning answering your crackpot arguments and I need some respite: S see you all later:)
 
What evidence?

My guess at your reasoning is as follows. Please don't be offended if I guessed wrong.

A) system X includes tunneling but, experimentally, doesn't radiate.
B) All systems that accelerate radiate.
C) Therefore system X doesn't accelerate.

If this is the reasoning, statement B is wrong so you can't conclude C from A.

But in a superconductor the experimental evidence is compelling that the charge-carriers are moving under conditions for which Ehrenfest's theorem does not apply. This must be so since when these charge-carriers move through a Josephson junction with a voltage-gradient, so that Ehrenfest's theorem does apply, they emit EM-radiation. When they move through the superconductor, they do not emit such radiation: This means that Ehrenfest's theorem does not apply:

Hey, I guessed right this time!

Johan, you cannot infer that "no radiation from superconductors" implies "Ehrenfest doesn't apply". There is no radiation from DC superconductors because Maxwell's Equations say so, acceleration or not.
 
Please explain to me why there is such discord amongst all you clever people.
Since you have cowards hiding behind anonymity who attack all new ideas without first studying all the relevant information in detail. They do this since new information threaten their sense of security. It has all along been the same through the ages.

At present it is worse than it ever has been. Not even Galileo was as viciously assaulted by his peers. I discuss the reasons for this in detail in my book. Just note how viciously I am attacked by cowards on this thread. Not one of them has even taken the time to study what I have done. They rather "imagine" what I am talking about since it is then easier to heap scorn without taking any responsibility.

Do I hide behind anonymity? No! If you want to claim that you know more than another person in a specific field, like Sol, Ziggurat, and Ben are doing on this thread, and you are not willing to come clean with who you are, and what you have achieved in the field; what a type of person are you? If I ever sink as low as that I will consider myself to be totally devoid of any integrity.
Now, perhaps a stupid question wrt the extra energy that Johan talks about, does the electron at the crest of the density wave not have more energy than the electron at the trough of the wave?
I am sorry but density waves do not play a role in superconductivity.
 
I am sorry but density waves do not play a role in superconductivity.

OK,
but my understanding now of a Josephson Junction is:

Apply a DC voltage to the junction.

The insulator starts to radiate a high frequency (in the GHz range.)

Now you have only applied DC to the junction, What mechanism is causing this wave energy to radiate, as the electrons must be tunneling or barrier hopping the insulator from each lateral superconductor leading to the electrons radiating GHZ frequencies.

According to the link I posted earlier, http://www.physorg.com/news189798601.html , an experiment was performed using the X-ray beam of SLAC's Stanford Synchrotron Radiation Lightsource on a high-temperature superconductor to reveal the material's electronic structure, and they posit that the electrons do not pair, but travel in a wave which they call a density wave.

They do however state that they do not understand this phenomenom.
Could you elucidate on the mechanism responsible for the junction radiating please.

Thanks.

ETA: Are the electrons travelling only in one direction, in both directions or are we only seeing the frequencies of the emitted photon energy?
 
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Do I hide behind anonymity? No! If you want to claim that you know more than another person in a specific field, like Sol, Ziggurat, and Ben are doing on this thread, and you are not willing to come clean with who you are, and what you have achieved in the field; what a type of person are you? If I ever sink as low as that I will consider myself to be totally devoid of any integrity.

First, remember this: You wandered in, by choice, to a circle of posters that you already know are anonymous. There is a "close window" button in your browser that will make us go away. If you strongly prefer interactions with real names and IRL reputations attached, there are plenty of other venues for you, including (say) physics conferences.

Regarding charge/acceleration/radiation, I have cited specific pages and equations in a Jackson, an extremely well-respected E&M textbook, which you may even own a copy of. I have not invoked my word or my reputation. Does the content of Jackson chapter 14 somehow depend on the reader's citation index?

Regarding energy conservation, likewise, have I made no claims whatsoever that aren't in standard Freshman textbooks. I have not invoked my word or my reputation. If I make a statement you don't believe, ask me for a citation and I will provide one.
 
ETA: Are the electrons travelling only in one direction, in both directions or are we only seeing the frequencies of the emitted photon energy?

My common sense tells me the electrons must be bi-directional to cause the insulator (antenna) to radiate at the required frequencies.
 
It doesn't matter what sort of potentials you think you cannot have, you still have a nonzero d2<x>/dt2 if the electrons are moving in a circle. You keep trying to claim that they can move in a circle without an acceleration, and I keep telling you that quantum mechanics says you're wrong. d2<x>/dt2 is nonzero in such an event.
you are claiming that electrons within a superconductor are moving along a circle while accelerating towards the center. Please prove experimentally that this is happening. You are the one who are making unsubstantiated claims; not I.

The fact remains that such an accelerating electron WILL emit EM radiation; and your silly arguments based on a rotating disc and Ben's "rope", do no change this experimental fact one iota. I asked you before to set up an experiment in which an electron moves around a circle owing to an electric field while accelerating towards the center without radiating. A few years ago they demonstrated electrons moving in this manner around a nucleus, and all the electrons radiated: They call these "atoms": "Rydberg atoms". So even this experimental information proves you wrong!
Except, of course, for all the experimental evidence demonstrating a changing current in a superconductor.
And you know that this is caused by acceleration? Wow you know more things that are not so than any other person I have ever met: Quite a distinction you know!
No, according to Ehrenfest's theorem, expectation values must obey Newtonian mechanics.
Please define "expectation value" . The latter concept is BS. Ehrenfest's theorem shows that the energy of an electron wave is its mass and that when you have a gradient in potential the force acts at the wave's center-of-mass, as we all know that it must from the time of Newton.
Not under certain conditions, but always.
It is not the case when an electron wave moves across a barrier to the other side.
Otherwise quantum mechanics is wrong, and you're not claiming it is.
Schroedinger's equation, although an approximation since it uses the electron's mass as input, instead of the solution, works well: The Copenhagen interpretation and all quantum physics based on probability amplitudes are, however, seriously flawed.
Tunnneling happens in agreement with Ehrenfest's theorem, yes.
So the electron-wave accelerates up along the barrier against the force? It cannot do this just as it cannot move through the barrier unless it scales the barrier by means of a quantum hop.
Nope, I agree that tunneling can and does occur.
But you believe that it is a paranormal process during which the electron wave can move to the other side without having the energy to do so? Is this correct?
I'm claiming Ehrenfest's theorem always applies to quantum mechanics, including tunneling scenarios.
How does acceleration applies during tunneling?
Any breakdown in Ehrenfest's theorem is synonymous with a breakdown in quantum mechanics.
Ehrenfest's theorem does not break down when the boundary conditions are such that the electron experiences a gradient in potential energy without any barriers preventing it from moving. But it sure as hell does not accelerate an electron wave through barrier as you are claiming that it does.
Nothing about Ehrenfest's theorem provides for any such exception.
I have not said that at all! Can you read English?
Well, no. One example of accelerating charges that radiate logically cannot prove that all accelerating charges radiate. But one example where accelerating charges do not radiate will disprove that. And I, and others, have given you such examples.
You have not given a single example where an electron being accelerated by an electric-field does not radiate. Stop lying!
The effect is easily understood (even at the time), even if the cause is not. Zero resistance in the absence of a Meissner effect is not superconductivity, it is perfect conductivity.
And when charge-carriers move by acceleration it is also not superconductivity but only perfect conductivity. BTW there is not a single compelling reason in the literature why superconduction might not be possible without a Meissner effect. Before you again distort what I am saying: I am NOT saying that superconduction without th Meissner effect is possible. I am only saying that there is not a single well founded reason why the Meissner effect must always accompany superconduction.
You're wrong. They interact (and thus scatter) along the direction of current motion as well.
Scattering by dissipating energy to their surroundings? You are again playing semantics: Scattering in the case when distinguishing superconduction from normal conduction, is the type of scattering that generates entropy. Do you know what the latter term means?
Furthermore, scattering doesn't have to dissipate kinetic energy. Coherent scattering (as in a diffraction experiment) involves no change in kinetic energy.
Again can you see how dishonest you are? You know very well that the scattering we are talking about involves dissipation of kinetic energy; but now to make another cheap shot, you play the idiot.
You claim it's nonsense, but the results predict exactly what occurs. The induced voltage accelerates electrons, creating a current that counter-acts the applied field. As the applied field is canceled, the voltage drops to zero, and no more acceleration. The current is then persistent, and does not continue to change.
So if the induced voltage does this while it is there, why does the voltage applied over two contacts not keep on doing the same as such a voltage does within a vacuum diode?
Because you think that gets you out of having to explain what contradicts your theory. But it won't work. The laws of physics aren't different under equilibrium, I've given you examples of equilibrium conditions which do what you claim could not be done,
You have not that I am aware of
and from the point of view of an individual electron, even your equilibrium conditions are not, in fact, in equilibrium at all.
It is quite clear that you do not understand what equilibrium conditions mean. It does not mean that each electrons is in equilibrium; it pertains the macro-condition. For example the gas molecules within a bottle move all the time but they are in equilibrium at a constant temperature. Have you ever heard of "thermodynamics"?
FINALLY!
Which means that voltages, AND electric fields, are not prohibited in a superconductor. And neither are accelerations.
There are no voltages and electric field driving the charge-carriers when an equilibrium current flows. When they are present you have non-equilibrium conditions and then you must have energy dissipation.
You keep saying this, and never backing it up. How do you get an electron to move in a circle with nonzero d2<x>/dt2?
You have not read my model but is arrogant enough to claim that I have not backed it up! Really why are you guys so despicable. I have quite a few times explained how it works in terms of Schroedinger's equation which is commensurate with Heisenberg's relationship between energy and time. But for some reason such simple physics is beyond your comprehension!

The current within a superconductor ring flows because the electrons make linear quantum hops around the hole. After each jump the electron is temporarily stationary, There is thus no continuous acceleration towards the center of the hole which requires EM radiation to occur. Is this too difficult to understand?
 
The fact remains that such an accelerating electron WILL emit EM radiation; and your silly arguments based on a rotating disc and Ben's "rope", do no change this experimental fact one iota. I asked you before to set up an experiment in which an electron moves around a circle owing to an electric field while accelerating towards the center without radiating. A few years ago they demonstrated electrons moving in this manner around a nucleus, and all the electrons radiated: They call these "atoms": "Rydberg atoms". So even this experimental information proves you wrong!

Keep racking them up: the Rydberg atom is not one of the nonradiating solutions. It is, rather, one of the radiating solutions, with the E and B fields varying in time.

Please define "expectation value" . The latter concept is BS.

Um. "Expectation value" is not some weird aspect of quantum interpretation---it the average of a set of single measurements. Are measurements BS? Is it BS to compute their average value?

(Schrodinger's Equation allows you to predict this average value, via a certain weighted integral that you seem not to like. Perhaps you think that that is BS. Huh.)

You have not given a single example where an electron being accelerated by an electric-field does not radiate. Stop lying!

I have---the stretchy rope example. You have heaped insults on this example but curiously you haven't pointed out any time-dependent term in its E or B fields. (Because there isn't one.)

Does it matter that the electron is "accelerated by an electric field"? If not, the spinning disk counterexample is still spinning. If it does matter, you owe me an apology, because you got very angry the last time I asked why you thought it mattered.
 

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