Abstract
In the Bridgman process, a single crystal is grown by the directional solidification of an initially molten semiconductor (melt) contained in a cylindrical ampoule. A crystal-growth experiment in an earthorbiting vehicle is subjected to residual accelerations (g-jitters) which drive an undesirable oscillatory buoyant convection in the melt. Since many molten semiconductors have electrical conductivities which are comparable to that of mercury, the magnitude of the buoyant convection is dramatically reduced by applying a magnetic field during crystal growth. The magnetic field can be produced by a permanent magnet or by a solenoid around the crystal-growth furnace. We treat the buoyant convection driven by periodic g-jitters whose direction is parallel to the axis of the ampoule. There is a non-uniform magnetic field which is axisymmetric around the ampoule axis. We compare the magnitudes and characteristics of the buoyant convections for various non-uniform magnetic fields to those for a uniform axial magnetic field. Fringing fields with the largest or smallest magnetic fiux density at the crystal-melt interface are considered.
Original language | English |
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DOIs | |
State | Published - 1996 |
Externally published | Yes |
Event | 34th Aerospace Sciences Meeting and Exhibit, 1996 - Reno, United States Duration: Jan 15 1996 → Jan 18 1996 |
Conference
Conference | 34th Aerospace Sciences Meeting and Exhibit, 1996 |
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Country/Territory | United States |
City | Reno |
Period | 01/15/96 → 01/18/96 |
Funding
This research was supported by the National Science Foundation under Grants CTS 94-19484 and CTS 95-0016N. The calculations were performed on the Convex C3880 supercomputer at the National Center for Supercomputer Applications at the University of Illinois at Urbana-Champaign.