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September 3, 2009 17:19
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High-order accurate solutions to acoustic-elastic interface problems | |
on adapted parallel meshes using a discontinuous Galerkin method | |
Lucas C. Wilcox [1] | |
Carsten Burstedde [1] | |
Georg Stadler [1] | |
Omar Ghattas [1,2,3,4] | |
[1] Institute for Computational Engineering and Sciences, The | |
University of Texas at Austin, Austin, TX 78712, USA | |
[2] Jackson School of Geosciences, The University of Texas at Austin, | |
Austin, TX 78712, USA | |
[3] Department of Mechanical Engineering, The University of Texas at | |
Austin, Austin, TX 78712, USA | |
[4] Institute for Geophysics, The University of Texas at | |
Austin, J.J. Pickle Research Campus, Austin, TX 78758, USA | |
The overall goal of the this research project is to create systematic, | |
rigorous, and scalable algorithms for global seismic waveform | |
inversion. The first step we took along this path was to create an | |
accurate solver for numerically simulating wave propagation | |
in materials with acoustic-elastic interfaces. We have chosen | |
a high-order method to effectively eliminate numerical dispersion | |
enabling simulations over many periods of the wave. The numerical | |
method uses a strain-velocity formulation allowing for acoustic and | |
elastic wave equations to be solve in the same framework. Careful | |
attention has been taken to develop a numerical flux to ensure that | |
the method remains high-order in the presence of material | |
discontinuities. A sketch of its derivation is given. To study the | |
numerical accuracy of the proposed method we compare with | |
reference solutions of classical interface problems, including Raleigh | |
waves, Lamb waves, Stoneley waves, Scholte waves, and Love waves. | |
In designing our numerical method we kept the goal of numerical | |
inversion in mind. The problem of inferring a medium from | |
observations of scattered waveforms is fundamentally a ill-posed | |
problem. Using a least-squares misfit of the waveform at discrete | |
locations is know to produce local minimum in the objective function. | |
One way to overcome this is to use grid continuation which requires | |
adaptive mesh refinement (AMR). Applying this to the global inverse | |
problem demands parallel scalability from the ground up. We show | |
numerical results with adaptive meshes of Earth models that display | |
the method's accuracy on curvilinear nonconforming meshes. Since | |
these simulation require large-scale computing we report | |
strong and weak parallel scaling results for mesh generation and | |
solution of the equations. |
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