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"Wavelets in Numerical Simulation of PDE"
Abstracts:
1. Adaptive wavelet representation and differenciation on block-structured grids
Margarete. O. Domingues
Instituto Nacional de Pesquisas Espaciais - LMO/CPTEC
margaret@cptec.inpe.br
Sônia. M. Gomes
Universidade Estadual de Campinas - IMECC
soniag@ime.unicamp.br
Lilliam. M. A. Díaz
Instituto de Cibernética Matemática y Física
This paper considers an adaptive finite difference scheme for the numerical
solution of evolution partial differencial equations. The computational domain
is formed by non-overlapping blocks. Each block is a uniform grid, but step
size may change from one block to another. The blocks are not predetermined,
but they are dinamically constructed according to the refinement needs of the
numerical solution. The decision over whether a block should be refined or unrefined
is taken by looking at the magnitude of wavelet coefficients of the numerical
solution on such block. The main objective of this paper is to establish a general
framework for the construction and operation on such adaptive block-grids in
2D. The algorithms and data structure are formulated by using abstract concepts
borrowed from quaternary trees. This procedure helps the understanding of the
method and its computational implementation. The ability of the method is demonstrated
by solving some typical test problems.
2. A Fully Adaptive Multiresolution Scheme for Shock Computations
Magda. K. Kaibara
Universidade Estadual Paulista - Depto. de Matemática
kaibara@fc.unesp.br
Sônia M. Gomes
Universidade Estadual de Campinas - IMECC
soniag@ime.unicamp.br
The scheme is based on Ami Harten's ideas, the main tools coming from wavelet
theory, in the framework of multiresolution analysis for cell averages. But
instead of evolving cell averages on the finest uniform level, we propose to
evolve the cell averages on the grid determined by the significant wavelet coefficients.
Typically, there are few cells in each time step, big cells on smooth regions,
and smaller ones close to irregularities of the solution. For the numerical
flux, we use a simple uniform central finite difference scheme, adapted to the
size of each cell. If any of the required neighboring cell averages is not present,
it is interpolated from coarser scales. But we switch to ENO scheme in the finest
part of the grids. To show the feasibility and efficiency of the method, it
is applied to a system arising in polymer-flooding of an oil reservoir. In terms
of CPU time and memory requirements, it outperforms Harten's multiresoltution
algorithm.
3. Implicit Discontinuous Galerkin Method With Wavelet-Based
Space Adaptivity
Jorge L. D. Calle
calle@commodity.com.br
Philippe R B Devloo
Universidade Estadual de Campinas - FEC
phil@fec.unicamp.br
Sônia M. Gomes
Universidade Estadual de Campinas - IMECC
soniag@ime.unicamp.br
In this paper, adaptivity in space is introduced to control the error in the
numerical solution of hyperbolic systems of conservation laws. The reference
numerical scheme is a new version of the Discontinuous Galerkin method, which
uses an implicit diffusive term in the direction of the streamlines, for stability
purposes. The decision whether to refine or to unrefine the grid in a certain
location is taken according to the magnitude of wavelet coefficients, which
are indicators of local smoothness of the numerical solution. This kind of information
is also used in adaptive choices of the artificial diffusion coefficient and
the kind of numerical flux adopted on cells' interfaces. Numerical solutions
of the nonlinear Euler equations illustrate the efficiency of the method.
José. E. Castilho
Universidade Federal de Uberlândia -Faculdade de Matemática
jecastilho@ufu.br
Sônia M. Gomes
Universidade Estadual de Campinas -IMECC
soniag@ime.unicamp.br
The study in this paper is devoted to the stability and consistency analyses
of an adaptive multilevel time discretization proposed by Bacry, Mallat and
Papanicolau. The main idea is to evolve the components in a multirresolution
representation of the numerical solution by means of an explicit algorithm,
adapting the time step according to each scale level. For a model problem,
and in the context of biorthogonal wavelets, it is proved that the stability
condition and consistency order are the same as in the original non-adapted
scheme.