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On Fri, 25 Jun 1999, Bob Sciamanda wrote:a
billb wrote:
If a copper disk is spun on axis and immersed in a uniform b-field
perpendicular to the face of the copper disk, and if the leads to
and alsostandard voltmeter are touched to the center of the spinning disk
difference.slid along its rim, the meter will measure a real potential
an EAccording to the voltmeter, the "radial e-field" is real. . . .
The EMF mechanism here is the QVxB "generator principle" force, not
charges willfield (I speak in YOUR lab frame). As in any circuit, surface
externalbuild up and produce an E field to drive the current around the
force.circuit, but the EMF force acting inside the armature is the QVxB
the(The E field of the surface charges will of course also exist inside
thearmature, but this is a "secondary" effect, and in fact will oppose
is nocurrent - all exactly as in a "standard" armature generator) There
"mystery" here (or there) [:)<
Aha, then I've found a big fuzzy spot in my understanding. . .
. . . It was mypoles of
understanding that VxB is itself an e-field: it is the same as the
relativistic e-field that an electron sees as it flys between the
a cyclotron magnet. Wrong?
and
If we build a spinning disk-magnet device and sit it on the lab bench,
the magnet is ceramic (nonconductor), then in the lab frame won't anearby
test-charge "see" an e-field caused by the spinning magnet? At the
surface of the spinning disk-magnet, won't this e-field be radial?
If we place a metal plate close to the spinning magnet and parallel toits
face, won't this radial e-field cause the charges of the metal plateto
redistribute themselves until they produce a cancelling e-field andthus
cease their motion?
by
If we reverse the situation and spin the metal plate while keeping the
magnet still, won't the charges in the metal plate STILL redistribute
themselves as above? (Here neglecting any Tolman-force motions caused
centripetal acceleration of mobile electrons in the metal.)
William J. Beaty SCIENCE HOBBYISTwebsite