Matrix: Fluorem/PR02R

Description: PR02R: 2D turbulent case. F. Pacull, Lyon, France

Fluorem/PR02R graph Fluorem/PR02R graph
(bipartite graph drawing) (graph drawing of A+A')


Fluorem/PR02R dmperm of Fluorem/PR02R

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  • download as a MATLAB mat-file, file size: 64 MB. Use UFget(2336) or UFget('Fluorem/PR02R') in MATLAB.
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    Matrix properties
    number of rows161,070
    number of columns161,070
    nonzeros8,185,136
    structural full rank?yes
    structural rank161,070
    # of blocks from dmperm457
    # strongly connected comp.457
    explicit zero entries0
    nonzero pattern symmetry 95%
    numeric value symmetry 0%
    typereal
    structureunsymmetric
    Cholesky candidate?no
    positive definite?no

    authorF. Pacull
    editorT. Davis
    date2010
    kindcomputational fluid dynamics problem
    2D/3D problem?yes

    Additional fieldssize and type
    bfull 161070-by-1
    xfull 161070-by-1

    Notes:

    CFD matrices from Francois Pacull, FLUOREM, in Lyon, France        
                                                                       
    We are dealing with CFD and more precisely steady flow             
    parametrization. The equations involved are the compressible       
    Navier-Stokes ones (RANS).  These matrices are real, square and    
    indefinite, they correspond to the Jacobian with respect the       
    conservative fluid variables of the discretized governing          
    equations (finite-volume discretization). Thus they have a         
    block structure (corresponding to the mesh nodes: the block        
    size is the number of variables per mesh node), they are not       
    symmetric (however, their blockwise structure has a high level     
    of symmetry) and they often show some kind of hyperbolic           
    behavior. They have not been scaled or reordered.                  
                                                                       
    They are generated through automatic differentiation of the        
    flow solver around a steady state. A right hand-side is also       
    given for each matrix: this represents the derivative of the       
    equations with respect to a parameter (of operation or shape).     
    Since they are generated automatically, they may have "silent"     
    variables: these are variables corresponding to an identity        
    submatrix associated with a null right hand-side, for example      
    one of the three velocity components in a 2D case, or the          
    turbulent variables in a "frozen" turbulence case.                 
                                                                       
    We believe that these matrices are good test cases when            
    studying preconditioning methods for iterative methods, such as    
    block incomplete factorization, or when studying domain            
    decomposition methods or deflation. They are actually being        
    studied by a few researchers in France regarding numerical         
    methods, through the LIBRAERO research project of the ANR (national
    research agency): ANR-07-TLOG-011.                                 
                                                                       
    Francois Pacull, Lyon, France.  fpacull at fluorem.com             
                                                                       
    Specific problem descriptions:                                     
        PR02R: 2D turbulent case                                       
        number of mesh nodes: 23010                                    
        block size: 7                                                  
        variables: [rho,rho*u,rho*v,rho*w,rho*E,rho*k,rho*omega]       
        (rho v is "silent", the third row and column in each block     
        can be removed)                                                
        matrix order: 161070                                           
        nnz: 8185136                                                   
        comments: This is a 2D turbulent case, dominated by            
        convection. The geometry is a RAE wing profile and the mesh    
        is C-shaped.                                                   
    

    Ordering statistics:result
    nnz(chol(P*(A+A'+s*I)*P')) with AMD82,852,254
    Cholesky flop count1.0e+11
    nnz(L+U), no partial pivoting, with AMD165,543,438
    nnz(V) for QR, upper bound nnz(L) for LU, with COLAMD138,682,781
    nnz(R) for QR, upper bound nnz(U) for LU, with COLAMD255,515,083

    For a description of the statistics displayed above, click here.

    Maintained by Tim Davis, last updated 12-Mar-2014.
    Matrix pictures by cspy, a MATLAB function in the CSparse package.
    Matrix graphs by Yifan Hu, AT&T Labs Visualization Group.