Interface conditions for electromagnetic fields
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Maxwell's equations describe the behavior of electromagnetic fields; electric field, magnetic field, electric flux density and magnetic flux density. The differential forms of these equations require that there's always an open neighbourhood around the point they're applied to, otherwise the vector fields E, D, B and H are not differentiable. In other words the medium must be continuous. On the interface of two different medium with different values for electrical permittivity and magnetic permeability that doesn't apply.
However the interface conditions for the elecromagnetic field vectors can be derived from the integral forms of Maxwell's equations.
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[edit] Interface conditions for electric field vectors
[edit] For electric flux density
where:
is normal vector from medium 1 to medium 2.
ρs is the surface charge between the media.
Therefore the normal component of D has a step of surface charge on the interface surface. If there's no surface charge on the interface, the normal component of D is continuous.
[edit] For electric field
where:
is normal vector from medium 1 to medium 2.
Therefore the tangential component of E is continuous across the interface.
[edit] Interface conditions for magnetic field vectors
[edit] For magnetic flux density
where:
is normal vector from medium 1 to medium 2.
Therefore the normal component of B is continuous across the interface.
[edit] For magnetic field
where:
is normal vector from medium 1 to medium 2.
is the surface current density between the two media.
Therefore the tangential component of H is continuous across the surface if there's no surface current present.
[edit] See also
[edit] References
- John R. Reitz,Frederick J. Milford, Robert W. Christy (1993). Foundations of Electromagnetic theory (4rd ed.). Addison-Wesley. ISBN 0-201-52624-7.