The Taylor-least squares (TLS) scheme, developed to solve the unsteady advection4iffusion equation for advection-dominated cases in one and two dimensions, is extended to three dimensions and applied to some 3D examples to demonstrate its accuracy. The serendipity Hermite element is selected as an i
Numerical analysis of a least-squares finite element method for the time-dependent advection–diffusion equation
✍ Scribed by R.C. Leal Toledo; V. Ruas
- Publisher
- Elsevier Science
- Year
- 2011
- Tongue
- English
- Weight
- 340 KB
- Volume
- 235
- Category
- Article
- ISSN
- 0377-0427
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✦ Synopsis
A mixed finite element scheme designed for solving the time-dependent advection-diffusion equations expressed in terms of both the primal unknown and its flux, incorporating or not a reaction term, is studied. Once a time discretization of the Crank-Nicholson type is performed, the resulting system of equations allows for a stable approximation of both fields, by means of classical Lagrange continuous piecewise polynomial functions of arbitrary degree, in any space dimension. Convergence in the norm of H 1 × H(div) in space and in appropriate senses in time applying to this pair of fields is demonstrated.
📜 SIMILAR VOLUMES
We consider a singularly perturbed advection-diffusion two-point boundary value problem whose solution has a single boundary layer. Based on piecewise polynomial approximations of degree k P 1, a new stabilized finite element method is derived in the framework of a variation multiscale approach. The