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

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M. BAUSE: Aspects <strong>of</strong> SUPG/PSPG and GRAD-DIV Stabilized Finite Element<br />

Approximation <strong>of</strong> Compressible Viscous Flow<br />

✬<br />

✫<br />

Aspects <strong>of</strong> SUPG/PSPG and GRAD-DIV Stabilized<br />

Finite Element Approximation <strong>of</strong> Compressible Viscous Flow<br />

Markus Bause<br />

<strong>Institut</strong> <strong>für</strong> Angewandte Mathematik, Universität Erlangen-Nürnberg<br />

Martensstr. 3, 91058 Erlangen<br />

bause@am.uni-erlangen.de<br />

In this contribution various aspects <strong>of</strong> a theoretical analysis and numerical study <strong>of</strong><br />

SUPG/PSPG and grad-div stabilized finite element approximations (cf. [3]) <strong>of</strong> steady<br />

and unsteady compressible isothermal viscous flow are addressed. After temporal discretization<br />

<strong>of</strong> the time variable by means <strong>of</strong> the implicit Euler method, the equations <strong>of</strong><br />

compressible viscous flow are solved by an iteration between a generalized Oseen problem<br />

for the velocity and a hyperbolic transport equation for the perturbation from the mean<br />

density (cf. [1]). Such a splitting-type approach seems attractive for computations because<br />

it <strong>of</strong>fers a reduction to simpler problems for which highly refined numerical methods either<br />

are known or can be built from existing discretization techniques for similar equations,<br />

and because <strong>of</strong> the guidance that can be drawn from an existence theory based on it.<br />

In the case <strong>of</strong> steady motions <strong>of</strong> a compressible viscous gas, decribed by the equations<br />

∇ · (ρv) = 0 , ρv · ∇v − µ∆v − (λ + µ)∇∇ · v + ∇p = ρf ,<br />

p = kρ , v|∂Ω = 0 ,<br />

�<br />

Ω ρ dx = M<br />

the iteration for solving this system reads as: Let ρ = 1 + σ. Put v0 = 0, σ0 = 0. For<br />

given vn, σn compute vn+1, σn+1 by<br />

(i) solving the generalized Oseen-system<br />

∇ · vn+1 = −∇ · (σnvn) ,<br />

(1 + σn)vn · ∇vn+1 + 1<br />

2 ∇ · ((1 + σn)vn)vn+1 − µ∆vn+1 + ∇πn+1 = (1 + σn)f ,<br />

vn+1|∂Ω = 0,<br />

�<br />

Ω πn+1 dx = 0<br />

(ii) and, then, solving the hyperbolic transport equation<br />

kσn+1 + (λ + 2µ)∇ · (σn+1vn+1) = πn+1 − µ∇ · vn+1 .<br />

For the approximation <strong>of</strong> the separated Oseen problem, SUPG/PSPG and grad-div stabilized<br />

higher order finite techniques based on LBB-stable elements are used and analyzed.<br />

The transport equation is discretized by SUPG stabilized finite element methods. Error<br />

estimates are provided. Numerical results for realistic steady and unsteady benchmark<br />

problems (driven cavity flow, flow over a backward facing step and DFG-benchmark) are<br />

given for a large scale <strong>of</strong> Reynolds numbers.<br />

References<br />

[1] M. Bause, J. G. Heywood, A. Novotny and M. Padula, On some approximation schemes<br />

for steady compressible viscous flow, J. Math. Fluid Mech., 5 (2003), pp. 201–230.<br />

[2] M. Bause, Stabilized finite element approximation <strong>of</strong> compressible viscous flow, to appear, <strong>2006</strong>.<br />

[3] T. Gelhard et al., Stabilized finite element schemes with LBB-stable elements for incompressible<br />

flow, J. Comput. Appl. Math. 177 (2005), pp. 243–267.<br />

Speaker: BAUSE, M. 72 <strong>BAIL</strong> <strong>2006</strong><br />

✩<br />

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