2019
DOI: 10.48550/arxiv.1912.09319
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Assembly of multiscale linear PDE operators

Abstract: In numerous applications the mathematical model consists of different processes coupled across a lower dimensional manifold. Due to the multiscale coupling, finite element discretization of such models presents a challenge. Assuming that only singlescale finite element forms can be assembled we present here a simple algorithm for representing multiscale models as linear operators suitable for Krylov methods. Flexibility of the approach is demonstrated by numerical examples with coupling across dimensionality g… Show more

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Cited by 2 publications
(2 citation statements)
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“…The mesh of Γ then consists of facets of T h , see also Figure 2.1. The linear systems are assembled using the multiscale library FEniCS ii [38], a module built on top of cbc.block [44] and the FEniCS framework [42].…”
Section: Remark 22 (Common Setup Of Experiments) Throughout the Paper...mentioning
confidence: 99%
“…The mesh of Γ then consists of facets of T h , see also Figure 2.1. The linear systems are assembled using the multiscale library FEniCS ii [38], a module built on top of cbc.block [44] and the FEniCS framework [42].…”
Section: Remark 22 (Common Setup Of Experiments) Throughout the Paper...mentioning
confidence: 99%
“…To discretize (4), we use lowest order (P2-P1) Taylor-Hood elements for the Stokes velocity and pressure, while piecewise quadratic elements (P2) were used for the Darcy pressure and piecewise constant elements (P0) for the Lagrange multiplier. Discretization is carried out in the FEniCS library [24], with coupling maps between the interface and domains and the fractional Laplacians being implemented by the extension FEniCS ii [25].…”
Section: Preliminariesmentioning
confidence: 99%