AbstractApplying a rotating magnetic field to an electrically conducting liquid, a Lorentz force is induced which generates a melt rotation of a certain angular velocity. A cylindrical gallium melt (aspect ratio 2.5) has been used as a model liquid. The melt has been heated from the bottom (Ra= 106) or from the top (Ra= −106) and the resulting temperature fluctuations in the melt have been measured in dependence on the rotating field strength (Bmax= 30 mT). In the case of the unstable gradient 0.8 mT are sufficient to dominate the buoyancy driven convection and to reduce the amplitude of the buoyancy caused temperature oscillations for more than one order of magnitude. At the same time, the fluctuation frequency increases with the field strength. In the case of the stabilizing temperature gradient, low amplitude/high frequency temperature fluctuations are generated by the rotating magnetic field, indicating the transition to a time‐dependent flow. In both cases we see an increase of the convective heat transport for magnetic inductions higher than approximately 5 m T.Applying the rotating magnetic field to the Bridgman growth of gallium doped germanium, the same behavior can be seen: Growing with a top‐seeded arrangement, the intensity of the dopant striations is decreased and their frequency is increased. Growing with a bottom‐seeded arrangement, the interface curvature changes from concave to convex and the flow becomes time‐