首页> 外文期刊>Journal of Computational Physics >Discrete calderon's projections on parallelepipeds and their application to computing exterior magnetic fields for frc plasmas
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Discrete calderon's projections on parallelepipeds and their application to computing exterior magnetic fields for frc plasmas

机译:离散Calderon在平行六面体上的投影及其在计算frc等离子体的外部磁场中的应用

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摘要

Confining dense plasma in a field reversed configuration (FRC) is considered a promising approach to fusion. Numerical simulation of this process requires setting artificial boundary conditions (ABCs) for the magnetic field because whereas the plasma itself occupies a bounded region (within the FRC coils), the field extends from this region all the way to infinity. If the plasma is modeled using single fluid magnetohydrodynamics (MHD), then the exterior magnetic field can be considered quasi-static. This field has a scalar potential governed by the Laplace equation. The quasi-static ABC for the magnetic field is obtained using the method of difference potentials, in the form of a discrete Calderon boundary equation with projection on the artificial boundary shaped as a parallelepiped. The Calderon projection itself is computed by convolution with the discrete fundamental solution on the three-dimensional Cartesian grid.
机译:将致密等离子体限制在场反向配置(FRC)中被认为是一种有前途的融合方法。此过程的数值模拟需要为磁场设置人工边界条件(ABC),因为等离子本身占据有界区域(在FRC线圈内),而磁场从该区域一直延伸到无穷远。如果使用单流体磁流体动力学(MHD)对等离子体进行建模,则可以将外部磁场视为准静态的。该场具有由拉普拉斯方程控制的标量势。磁场的准静态ABC使用差分电势方法获得,形式为离散的Calderon边界方程,在人工边界上的投影形状为平行六面体。 Calderon投影本身是通过对三维笛卡尔网格上的离散基本解进行卷积计算得到的。

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