Calculation of the Vector Potential of the Magnetic Field in a Nonconductive Medium during Floating Zone Melting

The vector potential of the magnetic field in a region between the induction coil, upper part of the floating zone, liquid film, feed rod, and protective shield has been determined in an axisymmetric problem of floating zone melting of a silicon cylinder 5–10 cm in radius. The boundary condition at infinity has been brought to some semicircle connecting the feed rod and protective shield and located at a sufficiently large distance from the coil, which has made it possible the problem to be treated in a finite region. This region has been conformally mapped onto a rectangle, in which the problem of determining the magnetic field vector potential has been solved. The problem reduces to solving Laplace’s equation for the only nonzero component of the vector potential $${A_\varphi }$$ , where $$\varphi $$ is the azimuthal angle, with first- or second-order boundary conditions on the rectangle sides. The proposed method can be used to evaluate the variable thickness and shape of the liquid film adjacent to the lower part of the feed rod and the hydrodynamic flow in the film.

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Publication Details

Journal
Journal of Applied Mechanics and Technical Physics
Published
2025-06-01
DOI
https://doi.org/10.1134/s002189442570004x
Primary Topic
Solidification and crystal growth phenomena
Type
article
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article

Calculation of the Vector Potential of the Magnetic Field in a Nonconductive Medium during Floating Zone Melting

Journal of Applied Mechanics and Technical Physics
Solidification and crystal growth phenomena
article

Calculation of the Vector Potential of the Magnetic Field in a Nonconductive Medium during Floating Zone Melting

article en

Abstract

The vector potential of the magnetic field in a region between the induction coil, upper part of the floating zone, liquid film, feed rod, and protective shield has been determined in an axisymmetric problem of floating zone melting of a silicon cylinder 5–10 cm in radius. The boundary condition at infinity has been brought to some semicircle connecting the feed rod and protective shield and located at a sufficiently large distance from the coil, which has made it possible the problem to be treated in a finite region. This region has been conformally mapped onto a rectangle, in which the problem of determining the magnetic field vector potential has been solved. The problem reduces to solving Laplace’s equation for the only nonzero component of the vector potential $${A_\varphi }$$ , where $$\varphi $$ is the azimuthal angle, with first- or second-order boundary conditions on the rectangle sides. The proposed method can be used to evaluate the variable thickness and shape of the liquid film adjacent to the lower part of the feed rod and the hydrodynamic flow in the film.

Journal of Applied Mechanics and Technical PhysicsVol. 66(3)
Lavrentyev Institute of Hydrodynamics (RU)
Openalex Percentile: Top 49%
Solidification and crystal growth phenomena
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