Boundary condition for Maxwell equations

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SUMMARY

The discussion centers on the boundary conditions necessary for the application of Maxwell's equations, specifically addressing the implications of adding constants to electric and magnetic fields. It highlights the significance of boundary conditions, such as Dirichlet and Neumann conditions, in defining field problems. The Sommerfeld Radiation Condition is identified as essential for ensuring uniqueness in free-space scenarios. Weng Cho Chew's "Fields and Waves in Inhomogeneous Media" is recommended for further exploration of these concepts.

PREREQUISITES
  • Understanding of Maxwell's equations
  • Familiarity with boundary conditions (Dirichlet and Neumann)
  • Knowledge of potential fields and their transformation from E and B fields
  • Basic concepts of electromagnetic wave propagation in inhomogeneous media
NEXT STEPS
  • Study the Sommerfeld Radiation Condition for uniqueness in electromagnetic problems
  • Explore Weng Cho Chew's "Fields and Waves in Inhomogeneous Media" for advanced boundary condition applications
  • Learn about Green's functions in the context of electromagnetic fields
  • Investigate the implications of discontinuous permeability and permittivity on boundary conditions
USEFUL FOR

Physicists, electrical engineers, and students of electromagnetism seeking to deepen their understanding of boundary conditions in Maxwell's equations and their applications in various media.

paweld
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It's obvious that if Maxwell equations are fulfilled by some E(x,y,z,t)
and B(x,y,z,t), they are also fullfiled by E(x,y,z,t)+ E_0
and B(x,y,z,t)+B_0, where E_0 and B_0
are constants. This freedom has physical significance as it changes the Lorentz force
which act on a charge. It implies that together with Maxwell equation we should
give some boundary condition. But unfortunately I can't find any book where they are
explicitly given (Dirichlet and Neumann boundary condition are most often introduced for
equation for potential not field).
 
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But the E and B fields CAN be transformed into their respective potential fields. That's why we only use potential and the Dirichlet/Neumann boundary conditions. In fact, in many instances, one applies the Green's function with the boundary conditions. That, in principle, should completely define the field problem.

Edit: er.. never mind. I just realized that you have a time-dependence field.

Zz.
 
It depends on the problem. If it is free-space, then there is an implicit requirement that the fields must go to zero at infinity for uniqueness to be guaranteed (Sommerfeld Radiation Condition). If you have a discontinuous permeability and/or permittivity then you can deduce the boundary conditions from the partial differential equations themselves.

Weng Cho Chew's "Fields and Waves in Inhomogeneous Media" discusses both.
 

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