Earnshaw's Theorem in Electrostatics
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If you have a question about this talk, please contact Harsha Hutridurga.
Earshaw’s Theorem (1842) is the subject of
Section 116 of Maxwell’s Treatise. It asserts
that charged bodies in an electrostatic field
cannot be in a position of stable equilibrium.
His and modern physics texts proofs
are interesting but not proofs.
For point charges the result was proved
by Kozlov in 1986. The case of dielectric and
perfectly conducting bodies is current work with
Gregoire Allaire. The interesting
cases are when the linearization is degenerate.
For dielectric and perfectly conduction bodies
we prove that this can occur only when the
electric field is constant on a neighborhood
of the body.
This talk is part of the Partial Differential Equations seminar series.
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