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Electrostatic & Magnetostatic Field Analysis

467 bytes added, 14:39, 18 May 2017
/* The Finite Difference Technique */
Two types of domain boundary conditions can be applied:
*Dirichlet boundary condition: ψ = k=const.*Neumann boundary condition: &partialpart;ψ = k= const. [[EM.Ferma]]'s default domain boundary condition for both the electrostatic and magnetostatic solvers is Dirichlet. At the interface between different material media, additional boundary conditions must be applied. These boundary conditions involve electric or magnetic field components. The field components can be expressed as partial derivatives of the potential, i.e. in the form of ∂ψ/∂x, ∂ψ/∂y or ∂ψ/∂z.
== 2D Quasi-Static Solution of TEM Transmission Line Structures ==
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