Cylshell/s3rmt3m3
FEM, cylindrical shell, graded tri. mesh w/ 1666 triangles. , R/t=1000
Name |
s3rmt3m3 |
Group |
Cylshell |
Matrix ID |
1611 |
Num Rows
|
5,357 |
Num Cols
|
5,357 |
Nonzeros
|
207,123 |
Pattern Entries
|
207,695 |
Kind
|
Structural Problem |
Symmetric
|
Yes |
Date
|
1997 |
Author
|
R. Kouhia |
Editor
|
R. Boisvert, R. Pozo, K. Remington, B. Miller, R. Lipman, R. Barrett, J. Dongarra |
Structural Rank |
5,357 |
Structural Rank Full |
true |
Num Dmperm Blocks
|
1 |
Strongly Connect Components
|
1 |
Num Explicit Zeros
|
572 |
Pattern Symmetry
|
100% |
Numeric Symmetry
|
100% |
Cholesky Candidate
|
yes |
Positive Definite
|
yes |
Type
|
real |
SVD Statistics |
Matrix Norm |
9.598608e+03 |
Minimum Singular Value |
3.998353e-07 |
Condition Number |
2.400640e+10
|
Rank |
5,357 |
sprank(A)-rank(A) |
0 |
Null Space Dimension |
0 |
Full Numerical Rank? |
yes |
Download Singular Values |
MATLAB
|
Download |
MATLAB
Rutherford Boeing
Matrix Market
|
Notes |
%
%FILE s3rmt3m3.mtx
%TITLE Cyl shell R/t=1000 grad trian mesh 1666 stab MITC3 elem with drill rot
%KEY s3rmt3m3
%
%
%CONTRIBUTOR Reijo Kouhia (reijo.kouhia@hut.fi)
%
%BEGIN DESCRIPTION
% Matrix from a static analysis of a cylindrical shell
% Radius to thickness ratio R/t = 1000
% Length to radius ratio R/L = 1
% One octant discretized with graded triangular mesh (1666 elements)
% element:
% facet-type shell element where the bending part is formulated
% using the stabilized MITC theory (stabilization paramater 0.4)
% the membrane part includes drilling rotations using
% the Hughes-Brezzi formulation with (regularizing parameter = G/1000,
% where G is the shear modulus)
% full 3-point integration
% --------------------------------------------------------------------------
% Note:
% The sparsity pattern of the matrix is determined from the element
% connectivity data assuming that the element matrix is full.
% Since this case the material model is linear isotropically elastic
% there exist some zeros.
% Since the removal of those zero elements is trivial
% but the reconstruction of the current sparsity
% pattern is impossible from the sparsified structure without any further
% knowledge of the element connectivity, the zeros are retained in this file.
% ---------------------------------------------------------------------------
%END DESCRIPTION
%
%
|