A new method for refractive index adaptive meshing based on grid interfacing at material boundaries in "nite-di!erence time-domain (FDTD) methods is presented. It allows highly e$cient simulation of structures consisting of homogeneous regions with large di!erences in refractive index, which are fre
The Finite Difference Based Fast Adaptive Composite Grid Method
β Scribed by P. J. J. Ferket
- Publisher
- John Wiley and Sons
- Year
- 1996
- Tongue
- English
- Weight
- 991 KB
- Volume
- 3
- Category
- Article
- ISSN
- 1070-5325
No coin nor oath required. For personal study only.
β¦ Synopsis
The fast adaptive composite grid (FAC) method is an iterative method for solving discrete boundary value problems on composite grids. McCormick introduced the method in [8] and considered the convergence behaviour for discrete problems resulting from finite volume element discretization on composite grids. In this paper we consider discrete problems resulting from finite difference discretization on composite grids. We distinguish between two obvious discretization approaches at the grid points on the interfaces between fine and coarse subgrids. The FAC method for solving such discrete problems is described. In the FAC method several intergrid transfer operators appear. We study how the convergence behaviour depends on these intergrid transfer operators. Based on theoretical insights, (quasi-)optimal intergrid transfer operators are derived. Numerical results illustrate the fast convergence of the FAC method using these intergrid transfer operators.
π SIMILAR VOLUMES
tion distortion; in our case, the finesse can be chosen to be 9 for K s 0.1, K s 0.1, β₯ s 0.15, β₯ s 0.15.
We propose a finite-difference algorithm for solving the time-dependent Ginzburg-Landau (TDGL) equation coupled to the appropriate Maxwell equation. The time derivatives are discretized using a second-order semi-implicit scheme which, for intermediate values of the Ginzburg-Landau parameter , allows
The lattice Boltzmann method is a microscopic-based approach for solving the fluid flow problems at the macroscopic scales. The presently popular method uses regularly spaced lattices and cannot handle curved boundaries with desirable flexibility. To circumvent such difficulties, a finite difference