1995
DOI: 10.1016/0022-0248(94)00732-2
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Buoyant convection during Czochralski silicon growth with a strong, non-uniform, axisymmetric magnetic field

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Cited by 10 publications
(1 citation statement)
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“…Since the thermocapillary convection and the centrifugal-pumping flow are confined to the top layer, they have no effect on the 0(1) temperature because any heat released by a radially inward flow is exactly balanced by the heat absorbed by the equal radially outward flow. Since the 0(1) temperature is continuous through the top layer, i.e., Tt(r, ) = T,(r, b) + O(Ha-'/2), the temperatures needed to compute the thermocapillary 8 or buoyant 9 ' 0 convection in the top layer are given by the core temperature at z = b. We used a Chebyshev Spectral Collocation method to solve for the coupled variables Bpo and T,.…”
mentioning
confidence: 99%
“…Since the thermocapillary convection and the centrifugal-pumping flow are confined to the top layer, they have no effect on the 0(1) temperature because any heat released by a radially inward flow is exactly balanced by the heat absorbed by the equal radially outward flow. Since the 0(1) temperature is continuous through the top layer, i.e., Tt(r, ) = T,(r, b) + O(Ha-'/2), the temperatures needed to compute the thermocapillary 8 or buoyant 9 ' 0 convection in the top layer are given by the core temperature at z = b. We used a Chebyshev Spectral Collocation method to solve for the coupled variables Bpo and T,.…”
mentioning
confidence: 99%