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The sidewall boundary condition is also drastically influencing the characteristics of the western boundary current simulated.
Truncation of unbounded domains via a nonreflecting boundary condition is also considered.
The perfectly matched layer (PML) absorbing boundary condition is also used with FDTD SBC to terminate the computational space.
The transparent boundary condition is also improved so that any exponential growth at a boundary is suppressed.
The present method of developing a radiation boundary condition is also applicable to higher order finite difference schemes.
This boundary condition is also written as a combination of single and double layer potentials so that the same approach can be used to compute it accurately.
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A sixth-order accurate symmetrical representation for the Neumann boundary condition was also developed.
Numerical results pertaining to the variation of the lowest eigenvalues (or stress singularities) for various wedge aperture angles of the material 1, subjected to the afore-mentioned wedge-side boundary condition, are also presented.
The dual results for the other integral boundary condition are also given.
The existence and exponential decay for a nonlinear wave equation with a nonlocal boundary condition were also proved in [9].
As an application, the existence of solutions for Laplace equations with a Neumann-type boundary condition was also proved, which has recently been used to study the Cauchy problem of Laplace equation by Wang [2].
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