The way in which induced or remanent magnetization contributes to the crust
al magnetic field at a point r on or above the Earth's surface is investiga
ted. It is shown that only smoothly varying components of magnetization alo
ng an azimuth phi about r contribute to the crustal magnetic field. Stated
mathematically, if the distribution of magnetization is expanded in a discr
ete Fourier basis in phi, only wavenumbers k=0, +/- 1, +/- 2 contribute to
the crustal field. On the other hand, there is no such simplifying expansio
n of the magnetization distribution in the radial direction. In the case wh
ere the induced magnetic field is due to a local variation of susceptibilit
y in a smooth inducing field such as the core field, this result can be ext
ended to the distribution of susceptibility itself. Then, when induced and
inducing magnetic field vectors are defined in the same local spherical sys
tem of coordinates, the matrix relating these two fields presents a very we
ll-defined and simple structure.