Abstract
We propose a method, which allows us to recover an optimal error convergence rate, when it is used in addition to the usual P1 Lagrange Finite Element Method, in 2d non-convex domains. It can be applied to the Laplace problem, the heat or wave equations, or similar problems with piecewise constant coefficients.
| Translated title of the contribution | La méthode du complément singulier pour des problèmes scalaires 2d |
|---|---|
| Original language | English |
| Pages (from-to) | 353-358 |
| Number of pages | 6 |
| Journal | Comptes Rendus Mathematique |
| Volume | 336 |
| Issue number | 4 |
| DOIs | |
| Publication status | Published - 15 Feb 2003 |