Abstract
In this paper, the technique of construction and analysis of quasimonotone finite-difference numerical schemes for scalar conservation laws in one space dimension, developed in Part I, is extended to a wide class of Petrov-Galerkin finite-element methods. The resulting schemes are called the quasimonotone finite-element schemes. The approximate solution is written as ūh + ūh, where ūh is a piecewise-constant function. The Petrov-Galerkin methods are then considered to be a set of equations that defines 'the parameter' ūh, plus a single equation, which is essentially a finite-difference scheme, that defines 'the means' ūh. All the results of the theory of quasimonotone finite-difference schemes can be carried over this finite-element framework by this simple point of view.
| Original language | English (US) |
|---|---|
| Pages (from-to) | 247-258 |
| Number of pages | 12 |
| Journal | SIAM Journal on Numerical Analysis |
| Volume | 27 |
| Issue number | 1 |
| DOIs | |
| State | Published - 1990 |
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