Eg on page 185 "...We have derived the magnetic field of a straight current by analyzing only the *electric* field of moving charges..." (Purcell's emphasis)
(boldface mine)
Even here, Purcell does not
define the magnetic field as a the relativistic portion of an electric field; he
derives it. The
meaning of "magnetic field" exists independantly of electricy and relativity.
Alexander is making a common engineer's mistake; he has confused "definition" with "law" or "theorem" or something similar. This is a very insidious mistake because one you internalize it, it is extremely difficult to comprehend anything where the incorrect internalized definition may actually be false.
In this case, he has internalized some facts about electrostatics and magnetostatics, and does not realize how specialized those hypotheses are.
I don't entirely doubt the possibility that the magnetic field may be redundant information; the Maxwell equations allow one to solve for the magnetic field at all times given the electric field at all times and the boundary condition of knowing the entire magnetic field at one particular time... I don't doubt it may be possible to develop an intelligent way to select the boundary condition to yield a unique solution for the magnetic field. The anomalous magnetic moment of various particles could possibly be explained away with current loops in LQG or ST as opposed to being an inherent property of a particle as demanded by the standard model.
But Alexander is blinded by
very special cases of electromagnetism to allow him to recognize this. Coulomb's law only applies to electrostatic fields. The Biot-Savart law only applies to magnetostatic fields. The
only situation where a static electromagnetic field remains static after applying a Lorentz boost is in the special case where all currents involved are parallel to the boost. (such as in Purcell's example with a straight current). Alexanders claims fall apart for dynamic electromagnetic fields.
In particular, a magnetodynamic field is divided into two parts, an induction field and a radiation field, while an electrodynamic field is divided into a retarded Coulomb field, two intermediate fields, and a radiation field.
Reference:
Electromagnetic Field Theory by Bo Thide, sections 7.1 and 7.2
http://www.plasma.uu.se/CED/Book/
In particular, the magnetic field at a point x in space is (where &rho, j, and a are evaluated at a retarded time allowing for light speed propagation from y to x, and letting r = x - y, and integration is over all of space)
B = (&mu0 / 4 &pi) &int j * r / r3 d3y + (&mu0 / 4 &pi c) &int j' * r / r2 d3y
Whereas the electric field is:
E = (1 / 4 &pi &epsilon0) &int &rho r / r3 d3y + (1 / 4 &pi &epsilon0 c) &int (j.r) r / r4 d3y
+ (1 / 4 &pi &epsilon0 c) &int (j * r) * r / r4 d3y + (1 / 4 &pi &epsilon0 c2) &int (j' * r) * r / r3 d3y
As you can see, the "law" B = v*E/c2 for the fields generated by volume elements only holds for the first term in each field (if we define v as j/&rho); the retarded coulomb field and the induction field. This law does not hold for the entire field! One piece of interest is that of the radiation field (the final terms). The radiative electric field of a volume element is best expressed in terms of the radiative magnetic field:
E = c B * r / r
This is far from the results predicted by extrapolating from the special case of boosting along a straight current.
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