We analyse the external field generated by a uniform distribution of magnet
ic susceptibility contained in an oblate spheroidal shell when it is magnet
ized by an internal magnetic field of arbitrary complexity. The situation i
s more relevant to the Earth than that of a spherical shell considered by R
uncorn (1975a) tin the context of lunar magnetism), because of the larger f
lattening of the Earth than that of the Moon. We find that, to first order
in the susceptibility, each internal harmonic in a spheroidal harmonic expa
nsion of the magnetic potential generates just one non-vanishing external f
ield coefficient: unlike in the spherical case when all harmonics vanish id
entically. The field generated is proportional to the susceptibility, thick
ness of the shell and square of the Earth's eccentricity, and hence it appe
ars that this field amplification mechanism will be very ineffective for th
e Earth.