A point generated incident field impinges upon a small triaxial ellipsoid w
hich is arbitrarily oriented with respect to the point source. The point so
urce field is so modified as to be able to recover the corresponding result
s for plane wave incidence when the source recedes to infinity. The main di
fficulty in solving analytically this low-frequency scattering problem conc
erns the fitting of the spherical geometry, which characterizes the inciden
t field, with the ellipsoidal geometry which is naturally adapted to the sc
atterer. A series of techniques has been used which lead finally to analyti
c solutions for the leading two low-frequency terms of the near as well as
the far field. In contrast to the near-field approximations, which are expr
essed in terms of ellipsoidal eigenexpansions, the far field is furnished b
y a finite number of terms. This is very interesting because the constants
entering the expressions of the Lame functions of degree higher than three
are not obtainable analytically and therefore, in the near field, not even
the Rayleigh approximation can be completely obtained. On the other hand, s
ince only a few terms survive at the far field, the scattering amplitude an
d the scattering cross-section are derived in closed form. It is shown that
, in practice, if the source is located a distance equal to five or six tim
es the biggest semiaxis of the ellipsoid the Rayleigh term of the approxima
tion behaves almost as the incident field was a plane wave. The special cas
es of spheroids, needles, discs, spheres as well as plane wave incidence ar
e recovered. Finally, some theorems concerning monopole and dipole surface
potentials are included.