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Inexact GMRES: Stokes equation

Version 3 2016-03-10, 15:49
Version 2 2016-03-10, 03:21
Version 1 2016-03-09, 02:28
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posted on 2016-03-10, 15:49 authored by Tingyu Wang, Simon K. Layton, Lorena A. BarbaLorena A. Barba
Figures and plotting scripts.

Figures 10–14 of the paper: "Inexact Krylov iterations and relaxation strategies with fast-multipole boundary element method"

Submitted for peer review.

Fig. 10: (StokesConvergence.pdf)
Convergence of the boundary-integral solution for Stokes flow around a sphere, using a  first-kind equation; p=16, linear system solved to 10^-5 tolerance. The relative error is with respect to the analytical solution for drag on a sphere.

Fig. 11: (StokesResidualHistory.pdf)
Residual history solving for surface traction on the surface of a sphere (first-kind integral problem), with a 10^-5 solver tolerance, 8,192 panels, and p=16 in the multipole expansions.

Fig. 12: (StokesSolveBreakdown.pdf)
Time breakdown between P2P and M2L when using a relaxation strategy for solving surface traction on the surface of a sphere, 10^-5 solver tolerance, 8,192 panels, p=16.

Fig. 13: (StokesSpeedupRelaxation.pdf)
Speed-up for solving first-kind Stokes equation on the surface of a sphere, varying N. 10^-5 solver tolerance, p=16.

Fig. 14: (StokesSpeedupTolerance.pdf)
Speed-ups for solving a 1st-kind Stokes problem on a sphere discretized with 8,192 panels, as the GMRES solver's tolerance increases; p=16 for all cases.

Funding

National Science Foundation award ACI-1149784

History