Q-reeus
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I can only repeat what has been put already. It is an experimental fact that ferromagnetic and ferrimagnetic media do not respond to an induced magnetic field as though composed of microscopic perfectly conducting classical loop currents. If it were so then net magnetic induction Btot within such media would attempt to be invariant, in keeping with the requirement that no electrical field exist within, or have a tangent component at the surface of, such conducting entities - only satisfied if the net flux enclosed within each such loop current is maintained constant (perfect diamagnetism - see e.g. www.phy.duke.edu/~hx3/physics/Superconductor2.pdf ). And that predicts a net media susceptibility -> - 1. [Magnitude would be somewhat less than unity owing to thermal jostling, and less than 100% achievable volume packing fraction of such loops] Does not happen that way. Actual susceptibilities can run into the hundreds of thousands for magnetically 'soft' media, while essentially zero for permanent magnets in their useful range of use. Quantum mechanics rules here and what is invariant is not enclosed flux within such hypothetical loop currents, but rather the magnitude of the intrinsic electron dipole moment.
To claim E.j work is being done on such intrinsic moments is inviting a severe paradox since, as touched on in #26 "there must somehow be some mysterious energy source which keeps the magnetic dipole moment constant when subjected to external field," (actually, time-changing B field giving rise to non-zero E.j) There is indeed something to this 'mysterious energy source' which bears further thought as per my closing bit in #53. At any rate, actually observed magnetic response, whether of permanent magnets or transformer cores etc., is best thought of in terms of fictitious magnetic dipoles of fixed magnitude - and that property cannot be explained via tiny classically behaving loop currents. And if one cannot then model using such loop currents, the whole argument that all energy exchanges are explained as E.j interactions simply fails.
For real situations there is finite conductivity and it's this generally quite minor induced eddy-current component that can be explained without controversy as E.j interactions. In the case of induced magnetization (e.g. example of soft iron paper-clip attracted to permanent magnet), there is a formal 'induced current' interaction but only in the sense of a varying magnetic moment m in F = ∇(m.B), the interaction being consistently best treated as fundamentally magnetic not electric.
To claim E.j work is being done on such intrinsic moments is inviting a severe paradox since, as touched on in #26 "there must somehow be some mysterious energy source which keeps the magnetic dipole moment constant when subjected to external field," (actually, time-changing B field giving rise to non-zero E.j) There is indeed something to this 'mysterious energy source' which bears further thought as per my closing bit in #53. At any rate, actually observed magnetic response, whether of permanent magnets or transformer cores etc., is best thought of in terms of fictitious magnetic dipoles of fixed magnitude - and that property cannot be explained via tiny classically behaving loop currents. And if one cannot then model using such loop currents, the whole argument that all energy exchanges are explained as E.j interactions simply fails.
For real situations there is finite conductivity and it's this generally quite minor induced eddy-current component that can be explained without controversy as E.j interactions. In the case of induced magnetization (e.g. example of soft iron paper-clip attracted to permanent magnet), there is a formal 'induced current' interaction but only in the sense of a varying magnetic moment m in F = ∇(m.B), the interaction being consistently best treated as fundamentally magnetic not electric.
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