Viscous fingering phenomenon in a linear channel is studied for a magnetic
fluid subjected to an external magnetic field. The competition between the
hydrodynamic effects and the capillary effects leads to the formation of an
interface between the air and the fluid which has a finger shape. It is th
e so-called Saffman-Taylor instability (STI). The influence of the magnetic
effects depends on the direction of the applied field: it is possible eith
er to enhance or to reduce the destabilizing phenomena. We study the onset
of the STI and compare the experimental results with the linear analysis in
cluding the magnetic contribution. In the nonlinear regime, the measurement
of the width of the finger as a function of the direction and the amplitud
e of the magnetic field is understood using a phenomenological approach. (C
) 2001 American Institute of Physics.