The Support Operator Rupture Dynamics (SORD) code simulates spontaneous rupture within a 3D isotropic viscoelastic solid. Wave motions are computed on a logically rectangular hexahedral mesh, using the generalized finite difference method of support operators. Stiffness and viscous hourglass corrections are employed to suppress suppress zero-energy grid oscillation modes. The fault surface is modeled by coupled double nodes, where the strength of the coupling is determined by a linear slip-weakening friction law. External boundaries may be reflective or absorbing, where absorbing boundaries are handled using the method of perfectly matched layers (PML). The hexahedral mesh can accommodate non-planar ruptures and surface topography
SORD simulations are configured with Python scripts. Underlying computations are coded in Fortran 95 and parallelized for multi-processor execution using Message Passing Interface (MPI) and OpenMP. The code is portable and tested with a variety of Fortran 95 compilers, MPI implementations, and UNIX-like operating systems (Linux, MacOS, IBM AIX, etc.).
The formulation, numerical algorithm, and verification of the SORD method are described by Ely, Day, and Minster (2008) for wave propagation, and Ely, Day, and Minster (2009) for spontaneous rupture. Ely, Day, and Minster (2010) present an application to simulating earthquakes in southern California.
Run a simple point source explosion test and plot a 2D slice of particle velocity:
cd scripts python SORD-Example-sim.py python SORD-Example-ploy.py
Plotting requires Matplotlib, and the result should look like this:
The general procedure is to import the
cst module, create a dictionary of parameters, and pass that dictionary to the
cst.sord.run() function. Parameters are either job-control or simulation parameters. Defaults for these two types of parameters are given in cst.job.defaults and cst.sord.parameters, respectively. Machine specific job-control parameters may also be present in the
conf directory that supersede the defaults.
It maybe be helpful to look through example applications in the
scripts directory, and return to this document for further description of the simulation parameters.
[Note about a change from previous versions: The
fieldio parameter has been removed, and instead each field I/O parameter is a separate list.]
Multi-dimensional field arrays may be accessed for input and out through a list of operations that includes reading from and writing to disk, as well as assigning to scalar values or time-dependent functions. In the quick test above,
v2 are examples of 3- and 4-D fields. The full list of available fields is given in the cst.sord.fieldnames dictionary.
Field variables are categorized in four ways: (1) static vs. dynamic, (2) settable vs. output only, (3) node vs. cell registration, and (4) volume vs. fault surface. For example, density
rho is a static, settable, cell, volume variable. Slip path length
sl is a dynamic, output, node, fault variable.
Field operations may specify a subregion of the array by giving slicing indices for each dimension. The 0-based indices can be either, a single index, empty brackets
 as shorthand for the entire array, of arguments to the python
slice() function, which can be either [start], [start, stop] or [start, stop, step]. Here are some examples:
[10, 20, 1, ] # Single cell, full time history [10, 20, 1, -1] # Single node, last time step [, , , -1] # Full 3D volume, last time step [10, , , [0, None, 10]] # j=10 node surface, every 10th time step
FIXME: this section is unfinished.
f = val # Set f to value f = (, '=', val) # Set f slice to value f = (, '+', val) # Add value to f slice f = (, '=', 'rand', val) # Random numbers in range (0, val) f = (, '=', 'func', val, tau) # Time function with period tau, scaled by val f = (, '<=', 'filename') # Read filename into f f = (, '=>', 'filename') # Write f into filename
A dot (
.) indicates sub-cell positioning via weighted averaging. In this case the spatial indices are single logical coordinates that may vary continuously over the range. The fractional part of the index determines the weights. For example, an index of 3.2 to the 1D variable f would specify the weighted average: 0.8 * f(3) + 0.2 * f(4).
Reading and writing to disk uses flat binary files where j is the fastest changing index, and t is the slowest changing index. Mode ‘R’ extrapolates any singleton dimensions to fill the entire array. This is useful for reading 1D or 2D models into 3D simulations, obviating the need to store (possibly very large) 3D material and mesh coordinate files.
For a list of available time functions, see the
time_function subroutine in util.f90. The routine can be easily modified to add new time functions. Time functions can be offset in time with the
tm0 initial time parameter.
Boundary conditions for the six faces of the model domain are specified by the parameters
bc1 (near-size, x, y, and z faces) and
bc2 (far-side, x, y, and x faces). The symmetry boundary conditions can be used to reduce computations for problems where they are applicable. These are not used for specifying internal slip boundaries. However, for problems with symmetry across a slip surface, the fault may be placed at the boundary and combined with an anti-mirror symmetry condition. The following BC types are supported:
free: Vacuum free-surface. Stress is zero in cells outside the boundary.
rigid: Rigid surface. Displacement is zero at the boundary.
+node: Mirror symmetry at the node. Normal displacement is zero at the boundary. Useful for a boundary corresponding to (a) the plane orthogonal to the two nodal planes of a double-couple point source, (b) the plane normal to the mode-III axis of a symmetric rupture, or (c) the zero-width axis of a 2D plane strain problem.
-node: Anti-mirror symmetry at the node. Tangential displacement is zero at the boundary. Useful for a boundary corresponding to (a) the nodal planes of a double-couple point source, (b) the plane normal to the mode-II axis of a symmetric rupture, or (c) the zero-width axis of a 2D antiplane strain problem.
+cell: Mirror symmetry at the cell. Same as type 1, but centered on the cell.
-cell: Anti-mirror symmetry at the cell. Same as type -1, but centered on the cell. Can additionally be used when the boundary corresponds to the slip surface of a symmetric rupture.
pml: Perfectly match layer (PML) absorbing boundary.
Example: a 3D problem with a free surface at Z=0, and PML absorbing boundaries on all other boundary faces:
shape = [50, 50, 50, 100] bc1 = ['pml', 'pml', 'free'] bc2 = ['pml', 'pml', 'pml']
Example: a 2D antiplane strain problem with PML absorbing boundaries. The number of nodes is 2 for the zero-width axis:
shape = [50, 50, 2, 100] bc1 = ['pml', 'pml', '-node'] bc2 = ['pml', 'pml', '-node']
Fault rupture always follows a surface of the (possibly non-planar) logical mesh. The orientation of the fault plane is defined by the
faultnormal parameter. This can be either 1, 2, or 3 corresponding to surfaces normal to the j, k, or l logical mesh directions. Any other value (typically 0) disables rupture altogether. The location of the rupture plane with in the mesh is determined by the
ihypo parameter, which has a dual purpose of also defining the nucleation point. So, the indices of the collocated fault double nodes are given by
int(ihypo[faultnormal]) + 1. For example, a 3D problem of dimensions 200.0 x 200.0 x 200.0, with a fault plane located at z = 100.0, and double nodes at l = (21, 22), may be set up as such:
delta = [5.0, 5.0, 5.0, 0.1] faultnormal = 3 shape = [41, 41, 42, 100] hypocenter = [20.0, 20.0, 20.5] bc1 = ['free', 'free', 'free'] bc2 = ['free', 'free', 'free']
For problems with symmetry across the rupture surface (where mesh and material properties are mirror images), the symmetry may be exploited for computational savings by using an appropriate boundary condition and solving the elastic equations for only one side of the fault. In this case, the fault double nodes must lie at the model boundary, and the and the cell-centered anti-mirror symmetry condition used. For example, reducing the size of the previous example to put the rupture surface along the far z boundary:
shape = [41, 41, 22, 100] hypocenter = [20.0, 20.0, 20.5] bc1 = ['free', 'free', 'free'] bc2 = ['free', 'free', '-cell']
Alternatively, put the rupture surface along the near z boundary:
shape = [41, 41, 22, 100] hypocenter = [20.0, 20.0, 1.5] bc1 = ['free', 'free', '-cell'] bc2 = ['free', 'free', 'free']
Further symmetries may present. If our previous problem has slip only in the x direction, then we may also use node-centered mirror symmetry along the in-plane axis, and node-centered anti-mirror symmetry along the anti-plane axis, to reduce computations eight-fold:
shape = [21, 21, 22, 100] hypocenter = [20.0, 20.0, 20.5] bc1 = ['free', 'free', 'free'] bc2 = ['anti-n', 'mirror-n', 'anti-c'
23 single precision (four-byte) memory variables are required per mesh point. On current hardware, computation time is on the order of the one second per time step per one million mesh points. SORD scalability has been benchmarked up to 64 thousand processors at ALCF.
Figure. Weak-scaling benchmarks.