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Autores principales: Wright, Jack K., Harsha, N. R. Sree, Garner, Allen L.
Formato: Preprint
Publicado: 2025
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Acceso en línea:https://arxiv.org/abs/2504.13435
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author Wright, Jack K.
Harsha, N. R. Sree
Garner, Allen L.
author_facet Wright, Jack K.
Harsha, N. R. Sree
Garner, Allen L.
contents Recent studies have applied variational calculus, conformal mapping, and point transformations to extend the one-dimensional SCLC from planar gaps to more complicated geometries. However, introducing a magnetic field orthogonal to the diode's electric field complicates these calculations due to changes in the electron trajectory. This paper extends a recent study that applied variational calculus to determine the SCLC for a cylindrical crossed-field diode to derive an equation that is valid for any orthogonal coordinate system. We then derive equations for the SCLC for crossed-field gaps in spherical, tip-to-tip, and tip-to-plane geometries that can be solved numerically. These calculations exhibit a discontinuity at the Hull cutoff magnetic field $B_H$ corresponding to the transition to magnetic insulation as observed analytically for a planar geometry. The ratio of the crossed-field SCLC to the nonmagnetic SCLC becomes essentially independent of geometry when we fix $δ= D/D_M > 0.6$, where $D$ is the canonical gap distance accounting for geometric effects on electric potential and $D_M$ is the effective gap distance that accounts for magnetic field and geometry. The solutions for these geometries overlap as $δ\to 1$ since the geometric corrections for electric potential and magnetic field match. This indicates the possibility of more generally accounting for the combination of geometric and magnetic effects when calculating $B_H$ and SCLC.
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spellingShingle A generalized framework for the critical current for a one-dimensional crossed-field gap in an orthogonal coordinate system
Wright, Jack K.
Harsha, N. R. Sree
Garner, Allen L.
Plasma Physics
Applied Physics
Recent studies have applied variational calculus, conformal mapping, and point transformations to extend the one-dimensional SCLC from planar gaps to more complicated geometries. However, introducing a magnetic field orthogonal to the diode's electric field complicates these calculations due to changes in the electron trajectory. This paper extends a recent study that applied variational calculus to determine the SCLC for a cylindrical crossed-field diode to derive an equation that is valid for any orthogonal coordinate system. We then derive equations for the SCLC for crossed-field gaps in spherical, tip-to-tip, and tip-to-plane geometries that can be solved numerically. These calculations exhibit a discontinuity at the Hull cutoff magnetic field $B_H$ corresponding to the transition to magnetic insulation as observed analytically for a planar geometry. The ratio of the crossed-field SCLC to the nonmagnetic SCLC becomes essentially independent of geometry when we fix $δ= D/D_M > 0.6$, where $D$ is the canonical gap distance accounting for geometric effects on electric potential and $D_M$ is the effective gap distance that accounts for magnetic field and geometry. The solutions for these geometries overlap as $δ\to 1$ since the geometric corrections for electric potential and magnetic field match. This indicates the possibility of more generally accounting for the combination of geometric and magnetic effects when calculating $B_H$ and SCLC.
title A generalized framework for the critical current for a one-dimensional crossed-field gap in an orthogonal coordinate system
topic Plasma Physics
Applied Physics
url https://arxiv.org/abs/2504.13435