Comments by "Dr Gamma D" (@DrDeuteron) on "How Special Relativity Makes Magnets Work" video.
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@drslump9314 no, but I use his equations. I am in complete agreement with J. All fields are sourced from charge, current, and their time derivatives on the past lightcone, in manner such the time derivative of one is the curl of the other. In this view, an EM wave is not a self sustaining propagation (which leads the incorrect view posted above: that E and B swap energy out of phase….they are ofc in phase in the far field), rather it’s just fields at a point in space time cause by sources on the past light cone, and that cause propagates away from the source at c.
I recently adopted this (classical) view after seeing too many comments about photons experiencing no time and questions about how they know to oscillate if they don’t have time. Ug. Not to mention all the misconceptions about the speed of propagation in media: the nonzero fields are caused by q, j, and their dots on the past light one, end of story.
Don’t even get me started on virtual photons and their pop sci description has confused many a layman
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@IdeasAboveStation Just look up "Lorentz transformation of EM field". The Lorentz scalars are the invariants of the electromagnetic 4-tensor:
(F_ab)(F_ ab)= -2(E^2-B^2)
(e_abcd)(F_ab)(F_cd) = -4E.B
The EM field strength tensor is:
F_ab = d_aA_b - d_bA_a
where the indices run over (t, x, y, z).
d = (d/dt, d/dx, d/dy, d/dz) is the covariant 4-derivate and A=(phi, A_x, A_y, A_z) is the 4-vector potential. Phi is electric scalar potential and A_i (i=x,y,z) is the magnetic vector potential.
In general, it's called "The covariant formulation of Maxwell's Equations".
The last ingredient is the 4-vector current density j_a = (rho, j_x, j_y, j_z), so it's charge density (rho) and standard current density (j). Since it transforms under Lorentz transformations, and so does "A", you are guaranteed to always satisfy Maxwell equation in any frame.
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@SK-ow4vw This is a thought experiment, not a description of holes in a semiconductor. That adds needless complexity.
It's best imagined as a linear 1D 'solid' lattice of N protons and N independent electrons with equal lab spacing at all times. It then becomes Bell's Spaceship Paradox with N spaceships.
The only way to understand it is to do the Lorentz transform, the results which I posted above. (It can be done, with plots, in 100 lines of python).
You can then use the E, B transformation rules, and verify it all works out, as it always does, b/c SR is internally consistent. But the electron spacing must be dilated in the cat frame relative to the lab frame, a la Bell's Spaceship Paradox where the string does indeed break.
In conclusion: do the Lorentz transform, it is of the form y = mx + b, a line: it's not as intimidating as it appears.
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@TheRetsehc Understand Bell's Spaceship paradox (where the space ships are two electrons), and all questions will be answer. Now, it did confuse professionals for a number of years.
The electrons all accelerate to "cat speed" simultaneously in the lab (wire) frame, so their lab spacing never changes and the wire is always neutral--by definition.
In any other frame, "simultaneous" is different. In the cat frame, the leading electrons accelerate 1st, and the lagging one last: the cat see them dilated by gamma (g).
The proton lattice is one physical object, so the cat sees it contracted by gamma (g) (see: Born Rigidity).
If the lab charge density is +q and -q, the total is q+(-q)=0, while the ` cat sees [+gq - q/g] = q(g-1/g) =
qg(1-1/g2) = qg(1 - (1-b2)) = qgb2
where b2 is b^2, and b is beta is v/c. With c=1, v=b.
The lab has E=0 (neutral) , and B=qv (moving charges is current), the transformation of those fields to the cat frame goes E' = g(E + v X B) -> g(0+v(qv)) = qgb2....the exact same factor.
It always works out.
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@fjarran4782 Neither. The quantum origins of electromagnetism is local gauge invariance. In this picture, the invariance of physics under a local phase change of the wavefunction of a charged (e) particle (A so-called U(1) gauge symmetry) is restored by replacing the derivative (read: kinetic momentum, p) with the covariant derivative (p-ieA)...aka the canonical momentum. A is then identified as (electric potential, magnetic vector potential). Math ppl say "A" is a connection on the manifold, and the gauge symmetry leads to conservation of charge.
The power of this way of thinking becomes evident when considering quantum chromodynamics, where the gauge symmetry is SU(3), and 'charge' now becomes a fundamental representation with 3 types of charges: red, green, blue (and their anti-charges). The single photon is replaced with 3^2-1=8 color/anti-color charged gluons. Likewise for the SU(2) symmetry of the weak interaction and the 2^2-1 = 3 vector boson, W+, W-, W0...but there are some Higgs shenanigans that mix the W0 with a photon-like B, leading to two states: the massless photon of electromagnetism and the heavier Z0. It's pretty wild stuff.
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