Equation [3] states that the tangential component of the magnetic field will be discontinous by the amount of surface current at the boundary (K). We will consider two different boundary conditions along the outside radius of the modeling domain shown above: the Magnetic Insulation (MI) boundary condition and the Perfect Magnetic Conductor (PMC) boundary condition.
Step 1 of the general boundary-problem …
We can't answer that because there are no existing magnetic charges to conduct. Recent advances and requirements in communication technologies have attracted great interest in PMC's and Casimir experiments involving … The skin depth as diverges - effectively all frequencies are ``static'' to a perfect conductor. Perfect conductor boundaries, Waveguides Problem: (a) Beginning with the free Maxwell equations in unbounded space, show that the propagation of an electromagnetic wave is transverse. The Magnetic Insulation condition can be physically interpreted as a boundary to a domain that has infinite electrical conductivity. A perfect conductor can move as much charge instantly as is required to cancel all fields inside. Let us consider for a moment what time dependent EM fields look like at the surface of a ``perfect'' conductor. That is, show that the electric and magnetic fields oscillate in a plane perpendicular to the direction of propagation and perpendicular to each other.
That is, Ht1 is the component of the magnetic field tangnetial to the material boundary just inside the region 1. Perfect magnetic conductor (PMC) boundary conditions are dual to the more familiar perfect electric conductor (PEC) conditions and can be viewed as the electromagnetic analog of the boundary conditions in the bag model for hadrons in QCD. This will differ from Ht2 (the tangential magnetic field just inside region 2) only if an electric current flows on the surface. This paper presents the implementations of perfect magnetic conductor (PMC) and perfect electric conductor (PEC) boundary conditions for efficient fundamental alternating-direction-implicit (ADI) and locally one-dimensional (LOD) finite-difference time-domain (FDTD). 9.1.3 Reflection from perfect conductors One of the simplest examples of a boundary value problem is that of a uniform plane wave in vacuum normally incident upon a planar perfect conductor at z ≥ 0, as illustrated in Figure 9.1.1(a). Boundary Conditions at a Conducting Surface: Skin Depth.
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