jeroen tromp computational seismology. governing equations equation of motion: boundary condition:...
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Governing Equations
Equation of motion:
Boundary condition:
Initial conditions:
Earthquake source:
Constitutive relationship (Hooke’s law):
Classic Tools
• Semi-analytical methods
– Layer cake models: reflectivity/discrete wave number
– Spherically symmetric models: normal modes
• Asymptotic methods
– Ray theory
– WKBJ theory
– Coupled modes
Strong Form
• Velocity-stress formulation (first-order PDEs, ):
• Second-order finite-difference method:
• Fourth-order finite-difference method:
• Challenges:– Boundary conditions– Numerical dispersion & anisotropy
Weak Form
• Weak form valid for any test vector• Boundary conditions automatically included• Source term explicitly integrated
Finite-fault (kinematic) rupture:
Finite Elements
Mapping from reference cube to hexahedral elements:
Volume relationship:
Jacobian of the mapping:
Jacobian matrix:
• Challenges:– Numerical anisotropy & dispersion– Mass lumping/implicit time stepping
Spectral Elements
Degree 4 GLL points:
GLL points are n+1 roots of:
The 5 degree 4 Lagrange polynomials:
Note that at a GLL point:
General definition:
Interpolation
Representation of functions on an element in terms of Lagrange polynomials:
Gradient on an element:
Integration
Integration of functions over an element based upon GLL quadrature:
• Integrations are pulled back to the reference cube• In the SEM one uses:
• interpolation on GLL points• GLL quadrature
Degree 4 GLL points:
The Diagonal Mass Matrix
Representation of the displacement:
Representation of the test vector:
Weak form:
Diagonal mass matrix:
• Integrations are pulled back to the reference cube• In the SEM one uses:
• interpolation on GLL points• GLL quadrature
Degree 4 Lagrange polynomials:
Degree 4 GLL points:
Parallel Implementation
Global mesh partitioning:
Cubed Sphere: 6 n mesh slices2
Regional mesh partitioning:
n x m mesh slices
June 12, 2005, M=5.1 Big Bear
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Soil-Structure Interaction (0.33 Hz)
Stupazini 2007
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Soil-Structure Interaction (1 Hz)
Stupazini 2007
QuickTime™ and aYUV420 codec decompressor
are needed to see this picture.
Recent & Current Developments
• Switch to a (parallel) “GEO”CUBIT hexahedral finite-element mesher– Topography & bathymetry– Major geological interfaces– Basins– Fault surfaces
• Use ParMETIS or SCOTCH for mesh partitioning & load-balancing
• 2D mesher & solver are ready (SPECFEM2D)
• Currently developing SPECFEM3D solver (elastic & poroelastic)
• Add dynamic rupture capabilities
SPECFEM3D Users Map
New V4.0 Mesh
Michea & Komatitsch
Four doublings:• below the crust• in the mid mantle• two in the outer core
Note: two-layer crust
SEM Implementation of Attenuation
Modulus defect:
Unrelaxed modulus:
Memory variable equation:
Equivalent Standard Linear Solid (SLS) formulation:
Anelastic, anisotropic constitutive relationship:
Attenuation (3 SLSs)Attenuation (3 SLSs)
Physical dispersion (3 SLSs)Physical dispersion (3 SLSs)
11/26/1999 Vanuatu shallow event50 s - 500 s benchmark
PREM benchmarks include:• Attenuation• Transverse isotropy• Self-gravitation (Cowling)• Two-layer crust
6/4/1994 Bolivia Deep Event10 s - 500 s benchmark
PREM benchmarks include:• Attenuation• Transverse isotropy• Self-gravitation (Cowling)• Two-layer crust