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BAIL 2006 Book of Abstracts - Institut für Numerische und ...

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G. MATTHIES, L. TOBISKA: Mass conservation <strong>of</strong> finite element methods for coupled<br />

flow-transport problems<br />

✬<br />

✫<br />

Mass conservation <strong>of</strong> finite element methods for coupled flow-transport<br />

problems<br />

Gunar Matthies 1 and Lutz Tobiska 2<br />

1 Fakultät <strong>für</strong> Mathematik, Ruhr-Universität Bochum<br />

2 <strong>Institut</strong> <strong>für</strong> Analysis <strong>und</strong> Numerik, Otto-von-Guericke-Universität Magdeburg<br />

We consider a coupled flow-transport problem in a bo<strong>und</strong>ed domain Ω ⊂ R d , d = 2,3. The<br />

system is described by the instationary, incompressible Navier–Stokes equations<br />

and the time-dependent transport equation<br />

ut − ν△u + (u · ∇)u + ∇p = f in Ω × (0,T],<br />

div u = 0 in Ω × (0,T],<br />

u = ub on ∂Ω × (0,T],<br />

u(0) = u 0<br />

in Ω,<br />

ct − ε△c + u · ∇c = g in Ω × (0,T],<br />

(cu − ε∇c) · n = cI u · n on Γ− × (0,T],<br />

ε∇c · n = 0 on Γ+ × (0,T],<br />

c(0) = c 0<br />

in Ω.<br />

Here, u and p denote the velocity and the pressure <strong>of</strong> the fluid, respectively, ν and ε are small<br />

positive numbers, c is the concentration, cI the concentration at the inflow bo<strong>und</strong>ary Γ− :=<br />

{x ∈ ∂Ω : u · n < 0}, and Γ+ := ∂Ω \ Γ−. We assume that ub is the restriction <strong>of</strong> a divergence<br />

free function onto the bo<strong>und</strong>ary ∂Ω. Note that the velocity u from the Navier–Stokes equations<br />

enters the transport equation as a convection field.<br />

Due to incompressibility constraint, the weak solution c <strong>of</strong> (2) satisfies the global mass<br />

conservation property<br />

� � � �<br />

d<br />

cdx + cIu · ndγ + cu · ndγ = g dx. (3)<br />

dt Ω Γ−<br />

Γ+<br />

Ω<br />

It is well-known [1], that the finite element solutions satisfy in general the incompressibility<br />

constraint and the global mass conservation property (3) only approximately.<br />

Different discretisation methods [2, 3, 4] for the instationary, incompressible Navier–Stokes<br />

equations and stabilised schemes for the transport problem like SDFEM will be studied numerically.<br />

References<br />

[1] C. Dawson, S. Sun, M. F. Wheeler, Compatible algorithms for coupled flow and transport.<br />

Comput. Methods Appl. Mech. Engrg., 193, 2565–2580 (2004).<br />

[2] G. Matthies, L. Tobiska, The inf-sup condition for the mapped Qk/P disc<br />

k−1 element in arbitrary<br />

space dimensions. Computing, 69, 119–139 (2002).<br />

[3] G. Matthies, L. Tobiska, Inf-sup stable non-conforming finite elements <strong>of</strong> arbitrary order<br />

on triangles. Numer. Math., 102, 293–309 (2005).<br />

[4] G. Matthies, Inf-sup stable nonconforming finite elements <strong>of</strong> higher order on quadrilaterals<br />

and hexahedra. Bericht Nr. 373, Fakultät <strong>für</strong> Mathematik, Ruhr-Universität Bochum<br />

(2005).<br />

Speaker: MATTHIES, G. 115 <strong>BAIL</strong> <strong>2006</strong><br />

1<br />

(1)<br />

(2)<br />

✩<br />

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