Resistor for the treatment of materials
AssigneeCommissariat a l'Energie Atomique
InventorsBernard Bechevet, Claude Calvat, Philippe Hugot, Gerard Basset
Life of this patent
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Abstract
A resistor for the treatment of materials, such as for the production of monocrystals by the planar resistor method includes an electrically conductive thin plate having a zone with a plurality of holes. With respect to an electric current flowing in the plate substantially parallel to its faces, the plate has lower electrical resistance in a peripheral area of said zone than in the central portion thereof.
Claims9
A resistor for the treatment of materials especially for the production of monocrystalline material and for purifying material by zone melting, said resistor comprising an electrically conductive thin heating plate having a heating surface for exposure to the material to be treated, a second surface opposite the heating surface and a crystallization zone encompassing a selected area of said plate and extending between said surfaces, means defining a plurality of through-holes extending from said heating surface to said second surface in said zone for passage through said plate in said zone of material melted by contact with said heating surface when said plate is heated electrically, said holes being positioned in said zone so that the plate, with respect to an electrical current flowing in said plate parallel to said surfaces, has an electrical resistance which is lower in a peripheral area of said zone than in the central portion thereof.
A method of treating a charge of material by zone melting comprising the steps of forming an electrically conductive thin heating plate with a crystallization zone containing a plurality of holes extending between opposite faces of said plate and with an electrical resistance which is lower in a peripheral area of said zone than in the central portion thereof, positioning said charge and a nucleus at said opposite faces of said plate in said zone, passing an electric current through said plate parallel to the faces thereof so as to heat said plate above the melting point of said charge material and displacing the charge and the plate relatively so that the charge material melts upon contact with the plate and passes through the holes in said plate and is subjected to a selected thermal gradient in said zone.
Dependencies are inferred from the claim text.