A conductor at potential V = 0 has the shape of an infinite plane except for a hemispherical bulge of radius a. A charge q is placed above the center of the bulge, a distance p from the plane. What is the force on the charge?
Let the z-axis be the symmetry axis.
Placing image charges -q at z = - p,
q' = -qR/p at z = R2/p and -q' = qR/p at z = -R2/p
on the z-axis makes the surface of the conductor an
equipotential surface. The field everywhere outside the conductor
is the same as that due to q and the image charges (uniqueness
theorem). The force on q therefore is
F = k(-q2/(4p2) + qq'/(p -
R2/p)2 - qq'/(p +
R2/p)2)k
= -kq2(1/(4p2) + 4R3p3/(p4 -
R4)2)k.
The charge is pulled towards the conductor.
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