zDarby wrote:Not just a law: When you move an electric field, you get a magnetic field.
I meant to say "electric charge" not "electric field".
johanfprins wrote:[...]when a solitary charge passes you by with a constant velocity there is also no magnetic field.
This is counter to what I thought I knew about experimental evidence. Can you site an experiment that shows this is the case? ... It is my understanding a solitary moving charge *does* exhibit a magnetic field. I could easily be wrong, but that's what I understood to be true. I shall try to find an example in experiment.
...
Maxwells equations are great! They perfectly describe what happens when two electric charges are moving compared to eachother. But they describe a law, not a theory. Which is to say, they describe
what happens, not
why.
When earlier I spoke of photons, I was quoting current physics dogma. As flawed as it is, current dogma does portray a why --a theory-- for the magnetic field. This theory was what I was describing. I think we all agree this theory is deeply flawed, but it
is a
theory and not just law.
What I'm asking is if you have a preferred theory --again, not a 'what' but a 'why'; or, if you prefer: not a description but an explanation-- for magnetic fields?
johanfprins wrote:It is different from the superconducting phase which I can extract from a diamond substrate by an anode in the sense that the latter phase is a single holistic wave. It is not different from the diamond substrates I can now manufacture where the phase consists of separate charge-carriers. However, both phases conduct by means of quantum fluctuations; and are thus in this sense the same.
Ok. just to make sure I understood you correctly:
Superconductivity in chilled mercury is the effect of a singular wave.
But superconductivity in your diamond substrate is of many different waves tunneling in concert, if not in unison.
Is that what you're saying?
johanfprins wrote:Since the critical temperature of my phases is above 500 celsius, there is not a strong enough magnetic field to make any difference.
Are you saying that you
did expose it to a magnetic field and nothing interesting happened? Or that you already knew nothing would happen and you
didn't expose it to a magnetic field?
johanfprins wrote:That has been done MANY times for superconducting metal rings and superconducting wires and proved correct. Why should I repeat it?
Well, first to be certain that what you expect to happen is, in fact, what happens. After all, when things don't do what you expect them to, that's when exciting new insights take place!
But, just as importantly, comparing the magnetic field strength and polarity to the flow of current will tell you what the relationship is between the charge carriers and the current. And you'll have measured the data experimentally, not calculated it theoretically. I got the impression you had already done this. Was I wrong?
~~~~~
Edit:
johanfprins wrote:I just saw your "LEFT-HAND" rule. How do you come to this? The current is ALWAYS "RIGHT-HAND" rule. Since when you take the current as negative or positive into the opposite direction you get the SAME polarity as determined by the "RIGHT-HAND" rule. "LEFT-HAND" rule? Maybe you should reread Feynman's lectures

Yeah. I don't know what the hell I was thinking when I wrote that. I'll chock it up to it being late, or something.
I go back to Feynman over and over again. I forget, then get confused and befuddled until I go back to his lectures and re-discover.