| Matrix properties | |
| number of rows | 74,062 |
| number of columns | 74,062 |
| nonzeros | 1,731,206 |
| structural full rank? | yes |
| structural rank | 74,062 |
| # of blocks from dmperm | 1 |
| # strongly connected comp. | 1 |
| entries not in dmperm blocks | 0 |
| explicit zero entries | 0 |
| nonzero pattern symmetry | symmetric |
| numeric value symmetry | 61% |
| type | complex |
| structure | unsymmetric |
| Cholesky candidate? | no |
| positive definite? | no |
| author | S.-H. Lee |
| editor | T. Davis |
| date | 2008 |
| kind | electromagnetics problem |
| 2D/3D problem? | yes |
Notes:
Jeffrey (Shih-Hao) Lee is a PhD student in the Center for Computational Electromagnetics, Univ. of Illinois at Urbana-Champaign. He is working on the development and application of the finite element method for analyzing antennas, high-frequency circuits, high-speed circuits, and so on. The governing equations are Maxwell's equations. The matrix results from the finite-element discretization of a bandpass microwave filter at 500 MHz. The first-order vector element is employed. The absorbing boundary condition is applied on the outer boundary of the structure for emulating the open space. The port boundary condition is applied on each port of the circuit for the truncating the computational domain and exciting the circuit. Due to these boundary conditions, the finite-element system matrix is complex.
| Ordering statistics: | AMD | METIS |
| nnz(chol(P*(A+A'+s*I)*P')) | 30,376,062 | 17,655,316 |
| Cholesky flop count | 4.4e+10 | 1.4e+10 |
| nnz(L+U), no partial pivoting | 60,678,062 | 35,236,570 |
| nnz(V) for QR, upper bound nnz(L) for LU | 71,971,769 | 45,213,573 |
| nnz(R) for QR, upper bound nnz(U) for LU | 135,637,784 | 91,066,663 |
Maintained by Tim Davis, last updated 17-May-2008.
Matrix pictures by cspy, a MATLAB function in the CSparse package.
Matrix graphs by Yifan Hu, AT&T Labs Visualization Group.