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Liquid metal free surfaces under AC magnetic fields. Y. Fautrelle EPM lab./CNRS/Grenoble Polytechnic Institute Outline: introduction static deformations surface motions conclusions. Context. Industrial : In metallurgical applications the free surface is the key-point :
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Liquid metal free surfaces under AC magnetic fields Y. Fautrelle EPM lab./CNRS/Grenoble Polytechnic Institute Outline: introduction static deformations surface motions conclusions
Context • Industrial : • In metallurgical applications the free surface is the key-point : • pollution (oxidation), inclusion entrapment • contact between melt and crucible • mass transfers and refining (degassing, alloying …) Scientific : full magnetohydrodynamic coupling
Static deformations • The electromagnetic pressure is responsible for a static free surface deformation : dome effect in induction furnaces axisymmetric shaping levitation butsymmetry breaking may occur according to the aspect ratio highly non-symmetric patterns
Static deformations (ACHF) Domes are oftenly axisymmetric static dome-shape deformation of an aluminium free surface under the effect of a AC magnetic field, f = 7.5 kHz, cold crucible melting
Static levitation (ACHF=15 kHz) titanium drop in a cold crucible (slighly unstable)
Static deformations (ACHF) Axisymmetric shaping : not at all ! “Static dome” in a semi-levitation cold crucible; the liquid is a nickel-base alloy; pool diameter is 60 mm, electric current frequency is 30 kHz
coil liquid metal drop 60 mm substrate Scheme of the apparatus
Static deformations of a flat gallium drop (ACHF) The free surface may take complex static shapes R = 3cm, f = 14 kHz B = 0 - 40 mT
Static deformations of a flat gallium drop (ACHF 14 kHz + ACLF 0.5 Hz)
Free surface motions (ACLF) • Low frequency magnetic fields generate various types of surface waves • Forced (axisymmetric) waves • Unstable (non-symmetric) resonant waves symmetry breaking digitation emulsion
gallium circular drop (ACLF=1.5 Hz)simple transition axisymmetric azimuthal B = 0.15 T
Stability diagram of a mercury drop f4 f5 f6 f7 Inductor current (A) Frequency (Hz)
gallium circular drop (ACLF + DC)the azimuthal instability is suppressed BDC = 1 - 2 T BAC = 1 - 15% BDC
gallium elongated drop (ACLF = 2Hz)simple transition saussage type
Increase of the perimeter A being almost constant, increase of the surface area occurs through an increase of the drop perimeter p thus let us consider the non-dimensional perimeter NB : for a circle p+ = 2p = 3.54 A
Evolution of the non-dimensional perimeter versus the coil current log (p+) 2/3 log (I)
A l Energy balance Magnetic energy : with vol = h a2, A p l Surface energy : thus :
conclusions AC magnetic fields may be destabilizing even at high frequencies It is possible to generate surface by resonant effects by single frequency systems by two frequency systems It is possible to create functions stirring emulsion DC magnetic field component is stabilizing