Numerical solution of electromagnetic field problems arise in high frequency - light current and low frequency - heavy current situations. Such problems are governed by Maxwell field equations in differential and integral form and their solution is dependent upon ht geometry, properties of the medium, and the boundary and initial conditions. Elliptic partial differential equations, such as the Laplace, poisson and Helmholtz equations, are associated with steady state phenomena, i.e., boundary value problems usually modeling closed or bounded solution regions. Parabolic equations are generally...
Numerical solution of electromagnetic field problems arise in high frequency - light current and low frequency - heavy current situations. Such proble...