In our FEA code we perform the rotations at the local level, before assembly so that it is easy to apply the boundary conditions, then unrotate locally after solution to get the usual Cartesian components.  Somehow this seems more efficient than doing this globally, but perhaps I am missing something.
-sanjay

On 5/31/21 9:33 AM, Matthew Knepley wrote:
On Mon, May 31, 2021 at 11:12 AM Stefano Zampini <[email protected] <mailto:[email protected]>> wrote:

    Mike

    as long as P is a sparse matrix with compatible rows and cols
    (i.e. rows(P)= cols(A) = rows (A)) , MatPtAP will compute the result.


Stefano and Mark are correct. This will work.

I implemented the same thing in my code in a different way. I put this transformation into the mapping between local and global vector spaces. The global degrees of freedom are the ones you want for boundary conditions (normal and tangential to the boundary), and I eliminate the ones that are constrained. The local degrees of freedom are the normal Caresian ones, and these are used for assembly. The map is used when I execute DMGlobalToLocal() and DMLocalToGlobal(). There is an example of me doing this in SNES ex71, Poiseuille flow in a tilted channel.

  Thanks,

      Matt

    Il giorno lun 31 mag 2021 alle ore 16:52 Mark Adams
    <[email protected] <mailto:[email protected]>> ha scritto:



        On Mon, May 31, 2021 at 9:20 AM Michael Wick
        <[email protected]
        <mailto:[email protected]>> wrote:

            Hi PETSc team:

            I am considering implementing a skew roller boundary
            condition for my elasticity problem. The method is based
            on this journal paper:
            http://inside.mines.edu/~vgriffit/pubs/All_J_Pubs/18.pdf
            <http://inside.mines.edu/~vgriffit/pubs/All_J_Pubs/18.pdf>

            Or you may find the method in the attached Bathe's slides,
            pages 9 -10.

            Roughly speaking, a (very) sparse matrix T will be created
            which takes the shape [ I, O; O, R], where R is a 3x3
            rotation matrix. And the original linear problem K U = F
            will be modified into (T^t K T) (T^t U) = T^t F. In doing
            so, one can enforce a roller boundary condition on a
            slanted surface.

            I think it can be an easy option if I can generate the T
            matrix and do two matrix multiplications to get T^t K T. I
            noticed that there is a MatPtAP function. Yet, after
            reading a previous discussion, it seems that this function
            is not designed for this purposes
            
(https://lists.mcs.anl.gov/pipermail/petsc-users/2018-June/035477.html
            
<https://lists.mcs.anl.gov/pipermail/petsc-users/2018-June/035477.html>).


        Yes, and no. It is motivated and optimized for a Galerkin
        coarse grid operator for AMG solvers, but it is a projection
        and it should be fine. If not, we will fix it.

        We try to test our methods of "empty" operators , but I don't
        know if MatPtAP has ever been tested for super sparse P. Give
        it a shot and see what happens.

        Mark


            I assume I can only call MatMatMult & MatTransposeMatMult
            to do this job, correct? Is there any existingly PETSc
            function to do T^t K T in one call?

            Thanks,

            Mike



-- Stefano



--
What most experimenters take for granted before they begin their experiments is infinitely more interesting than any results to which their experiments lead.
-- Norbert Wiener

https://www.cse.buffalo.edu/~knepley/ <http://www.cse.buffalo.edu/~knepley/>

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