3−D Surface Topography Boundary Conditions in Seismic Wave Modelling

New alternative formulations of exact boundary conditions for arbitrary three{dimensional (3−D) free surface topographies on seismic media have been derived. They are shown to be equivalent with previously published formulations, thereby serving as a verification of the validity of each set of formu...

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Main Authors: Hestholm, Stig, Ruud, Bent
Other Authors: Massachusetts Institute of Technology. Earth Resources Laboratory
Format: Report
Language:unknown
Published: Massachusetts Institute of Technology. Earth Resources Laboratory 2001
Subjects:
Online Access:http://hdl.handle.net/1721.1/68608
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spelling ftmit:oai:dspace.mit.edu:1721.1/68608 2023-05-15T15:55:50+02:00 3−D Surface Topography Boundary Conditions in Seismic Wave Modelling Hestholm, Stig Ruud, Bent Massachusetts Institute of Technology. Earth Resources Laboratory Hestholm, Stig 2001 application/pdf http://hdl.handle.net/1721.1/68608 unknown Massachusetts Institute of Technology. Earth Resources Laboratory Earth Resources Laboratory Industry Consortia Annual Report;2001-13 http://hdl.handle.net/1721.1/68608 Technical Report 2001 ftmit 2020-10-28T08:27:11Z New alternative formulations of exact boundary conditions for arbitrary three{dimensional (3−D) free surface topographies on seismic media have been derived. They are shown to be equivalent with previously published formulations, thereby serving as a verification of the validity of each set of formulations. The top of a curved grid represents the free surface topography while the grid's interior represents the physical medium. We assume the velocity{stress version of the viscoelastic wave equations to be valid in this grid before transforming the equations to a rectangular grid. In order to do the numerical discretization we apply the latter version of equations for seismic wave propagation simulation in the interior of the medium. The numerical discretization of the free surface topography boundary conditions by second−order finite−differences (F−Ds) is shown in detail, as well as spatially unconditional stability of the resulting system of equations. The F−D order is increased by two for each point away from the free surface up to eight, which is the order used in the interior. We use staggered grids both in space and time and the second-order leap-frog and Crank-Nicholson methods for wave field time propagation. We simulate point sources at the surface of a homogeneous medium, with a plane surface containing a hill and a trench, respectively. The main features of these general cases are outlined. Then, we present results using parameters typical of teleseismic earthquakes and explosions with a 200 × 100 km[superscript 2] area of real topography from southwestern Norway over a homogeneous medium. A dipping plane wave simulates a teleseismic P−wave incident on the surface topography. Results show clear conversion from P− to Rg− (short period fundamental mode Rayleigh) waves in the steepest and/or roughest topography, as well as attenuated waves in valleys and fjords. The codes are parallellized for simulation on fast supercomputers to model higher frequencies and/or larger areas than before. Research Council of Norway Massachusetts Institute of Technology. Earth Resources Laboratory United States. Army. Corps of Engineers (contract DACA89-99-C-0002) Cold Regions Research and Engineering Laboratory (U.S.) Report Cold Regions Research and Engineering Laboratory DSpace@MIT (Massachusetts Institute of Technology) Nicholson ENVELOPE(78.236,78.236,-68.612,-68.612) Norway
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collection DSpace@MIT (Massachusetts Institute of Technology)
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language unknown
description New alternative formulations of exact boundary conditions for arbitrary three{dimensional (3−D) free surface topographies on seismic media have been derived. They are shown to be equivalent with previously published formulations, thereby serving as a verification of the validity of each set of formulations. The top of a curved grid represents the free surface topography while the grid's interior represents the physical medium. We assume the velocity{stress version of the viscoelastic wave equations to be valid in this grid before transforming the equations to a rectangular grid. In order to do the numerical discretization we apply the latter version of equations for seismic wave propagation simulation in the interior of the medium. The numerical discretization of the free surface topography boundary conditions by second−order finite−differences (F−Ds) is shown in detail, as well as spatially unconditional stability of the resulting system of equations. The F−D order is increased by two for each point away from the free surface up to eight, which is the order used in the interior. We use staggered grids both in space and time and the second-order leap-frog and Crank-Nicholson methods for wave field time propagation. We simulate point sources at the surface of a homogeneous medium, with a plane surface containing a hill and a trench, respectively. The main features of these general cases are outlined. Then, we present results using parameters typical of teleseismic earthquakes and explosions with a 200 × 100 km[superscript 2] area of real topography from southwestern Norway over a homogeneous medium. A dipping plane wave simulates a teleseismic P−wave incident on the surface topography. Results show clear conversion from P− to Rg− (short period fundamental mode Rayleigh) waves in the steepest and/or roughest topography, as well as attenuated waves in valleys and fjords. The codes are parallellized for simulation on fast supercomputers to model higher frequencies and/or larger areas than before. Research Council of Norway Massachusetts Institute of Technology. Earth Resources Laboratory United States. Army. Corps of Engineers (contract DACA89-99-C-0002) Cold Regions Research and Engineering Laboratory (U.S.)
author2 Massachusetts Institute of Technology. Earth Resources Laboratory
Hestholm, Stig
format Report
author Hestholm, Stig
Ruud, Bent
spellingShingle Hestholm, Stig
Ruud, Bent
3−D Surface Topography Boundary Conditions in Seismic Wave Modelling
author_facet Hestholm, Stig
Ruud, Bent
author_sort Hestholm, Stig
title 3−D Surface Topography Boundary Conditions in Seismic Wave Modelling
title_short 3−D Surface Topography Boundary Conditions in Seismic Wave Modelling
title_full 3−D Surface Topography Boundary Conditions in Seismic Wave Modelling
title_fullStr 3−D Surface Topography Boundary Conditions in Seismic Wave Modelling
title_full_unstemmed 3−D Surface Topography Boundary Conditions in Seismic Wave Modelling
title_sort 3−d surface topography boundary conditions in seismic wave modelling
publisher Massachusetts Institute of Technology. Earth Resources Laboratory
publishDate 2001
url http://hdl.handle.net/1721.1/68608
long_lat ENVELOPE(78.236,78.236,-68.612,-68.612)
geographic Nicholson
Norway
geographic_facet Nicholson
Norway
genre Cold Regions Research and Engineering Laboratory
genre_facet Cold Regions Research and Engineering Laboratory
op_relation Earth Resources Laboratory Industry Consortia Annual Report;2001-13
http://hdl.handle.net/1721.1/68608
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