We calculate the effect of a strong dipole magnetic field on non-axisymmetr
ic oscillations for roAp stars, with a typical range of photospheric magnet
ic fields B-p [0.5-1.5] kG. As Dziembowski & Goode (1996), we find that the
oscillations art strongly affected by such magnetic fields in two differen
t ways. The first one concerns the stability of modes, which are damped due
to dissipation by Alfvenic waves. It leads to a small imaginary part of th
e frequency, about (1-15 mu Hz). The real part of the frequencies is also a
ffected and is greater in the presence of magnetic field, with a shift of a
bout 1-20 mu Hz. We find that these shifts are strongly influenced by the g
eometry of the mode, i.e. the value of the degree l, as it has already been
shown by Dziembowski & Goode (1996), and also by m, the azimuthal degree,
with a significant amplitude. The magnetic field, because it breaks the sph
erical symmetry of the problem, raises partially the (2l + 1) degeneracy of
frequency in m. We find that the shift of both the real and imaginary part
s is always greater than in the case of axisymmetric oscillations (m = 0),
except for sectoral modes (l = m), for which the imaginary part is smaller
The second effect of large magnetic fields is to complicate the mode identi
fication. The perturbations cannot be represented by pure single spherical
harmonic, but by a series of harmonics due to the angular dependence of the
Lorentz force. it is shown that this mixing of spherical harmonics also de
pends on the value of m. However, our calculations do not explain the obser
ved selection of dipole modes in roAp stars, aligned with the magnetic axis
, since they do not minimize energy losses due to Alfvenic waves.