Sinclair/3Dspectralwave2
3-D spectral-element elastic wave modelling in freq. domain, C. Sinclair, Univ. Adelaide
| Name |
3Dspectralwave2 |
| Group |
Sinclair |
| Matrix ID |
1857 |
|
Num Rows
|
292,008 |
|
Num Cols
|
292,008 |
|
Nonzeros
|
12,935,272 |
|
Pattern Entries
|
14,322,744 |
|
Kind
|
Materials Problem |
|
Symmetric
|
No |
|
Date
|
2007 |
|
Author
|
C. Sinclair |
|
Editor
|
T. Davis |
| Structural Rank |
292,008 |
| Structural Rank Full |
true |
|
Num Dmperm Blocks
|
1 |
|
Strongly Connect Components
|
1 |
|
Num Explicit Zeros
|
1,387,472 |
|
Pattern Symmetry
|
100% |
|
Numeric Symmetry
|
100% |
|
Cholesky Candidate
|
yes |
|
Positive Definite
|
no |
|
Type
|
complex |
| Download |
MATLAB
Rutherford Boeing
Matrix Market
|
| Notes |
The A matrix is produced using 3-D spectral-element elastic wave modelling in
the frequency domain.The medium is homogeneous and isotropic with elastic
coefficients: c11 = 6.30, c44 = 1.00. The B matrix contains only one non-zero
entry, representing a real y-directed source, placed approximately in the
centre. The model size in elements is 10x10x10. Each element is 1m x1m x 1m.
Each element is a 4x4x4 Gauss-Lobbato-Legendre mesh, so the height, width and
depth of the system is 31 nodes. There are 3 unknown complex components at
each node - the x, y and z displacements. The A matrix therefore has
dimension 89373 x 89373. ((10 x 4) - (10 - 1))^3 * 3 = 89373. The solution
will consist of x-z planes. Note that A is complex and b is sparse and real
(b has a single nonzero).
The A matrix was provided with a nonzero imaginary part, but was otherwise
complex Hermitian. To save space in the Matrix Market and Rutherford/Boeing
formats, the A matrix here has had this imaginary diagonal removed. The
shift can be found in the aux.shift auxiliary matrix. To reproduce the
original A matrix, use A = Problem.A + Problem.aux.shift ;
|