P. Dold et Kw. Benz, MODIFICATION OF FLUID-FLOW AND HEAT-TRANSPORT IN VERTICAL BRIDGMAN CONFIGURATIONS BY ROTATING MAGNETIC-FIELDS, Crystal research and technology, 32(1), 1997, pp. 51-60
Applying a rotating magnetic field to an electrically conducting liqui
d, a Lorentz force is induced which generates a melt rotation of a cer
tain angular velocity. A cylindrical gallium melt (aspect ratio 2.5) h
as been used as a model liquid. The melt has been heated from the bott
om (Ra=10(6)) or from the top (Ra=-10(6)) and the resulting temperatur
e fluctuations in the melt have been measured in dependence on the rot
ating field strength (B-max=30 mT). In the case of the unstable gradie
nt 0.8 mT are sufficient to dominate the buoyancy driven convection an
d to reduce the amplitude of the buoyancy caused temperature oscillati
ons for more than one order of magnitude. At the same time. the fluctu
ation frequency increases with the field strength. In the case of the
stabilizing temperature gradient: low amplitude/high frequency tempera
ture fluctuations are generated by the rotating magnetic field, indica
ting the transition to a time-dependent flow. In both cases we see an
increase of the convective heat transport for magnetic inductions high
er than approximately 5 mT. Applying the rotating magnetic field to th
e Bridgman growth of gallium doped germanium, the same behavior can be
seen: Growing with a top-seeded arrangement, the intensity of the dop
ant 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-dependent.