Boundary condition for Maxwell equations

In summary, the conversation discusses the physical significance of the freedom to add constants to the electric and magnetic fields while still satisfying Maxwell's equations. This freedom requires the inclusion of boundary conditions for a complete description of the fields. However, the speaker mentions that it is difficult to find explicit boundary conditions for the fields, as they are often only given for potential equations. The use of potential fields and the Green's function with boundary conditions is also mentioned. The need for boundary conditions is further emphasized in the case of time-dependent fields. The conversation also touches on the use of discontinuous permeability and permittivity to determine boundary conditions.
  • #1
paweld
255
0
It's obvious that if Maxwell equations are fulfilled by some [tex] E(x,y,z,t)[/tex]
and [tex] B(x,y,z,t)[/tex], they are also fullfiled by [tex] E(x,y,z,t)+ E_0[/tex]
and [tex] B(x,y,z,t)+B_0[/tex], where [tex] E_0[/tex] and [tex] B_0[/tex]
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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  • #2
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.
 
  • #3
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.
 

Related to Boundary condition for Maxwell equations

1. What are boundary conditions for Maxwell's equations?

Boundary conditions for Maxwell's equations are the set of conditions that must be satisfied at the interface between two different materials or regions, in order for the equations to accurately describe the electromagnetic behavior at that boundary.

2. Why are boundary conditions important for Maxwell's equations?

Boundary conditions are important for Maxwell's equations because they allow us to accurately model the behavior of electromagnetic fields at interfaces, which are crucial for many practical applications such as antennas, waveguides, and optical devices.

3. What types of boundary conditions are there for Maxwell's equations?

There are two main types of boundary conditions for Maxwell's equations: electric boundary conditions and magnetic boundary conditions. Electric boundary conditions specify the behavior of the electric field at the interface, while magnetic boundary conditions specify the behavior of the magnetic field.

4. How are boundary conditions for Maxwell's equations determined?

Boundary conditions for Maxwell's equations are determined by the properties of the materials or regions that are in contact at the interface. These properties include the dielectric constant, magnetic permeability, and conductivity, which affect the behavior of the electromagnetic fields at the boundary.

5. Can boundary conditions for Maxwell's equations change?

Yes, boundary conditions for Maxwell's equations can change if the properties of the materials or regions at the interface change. For example, if the dielectric constant of a material changes, the electric boundary conditions at the interface will also change, resulting in a different behavior of the electromagnetic fields at that boundary.

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