> In step-7
>
>
https://www.dealii.org/current/doxygen/deal.II/step_7.html
> <
https://nam01.safelinks.protection.outlook.com/?url=https%3A%2F%2Fwww.dealii.org%2Fcurrent%2Fdoxygen%2Fdeal.II%2Fstep_7.html&data=02%7C01%7CWolfgang.Bangerth%40colostate.edu%7C95a7523f571844a4dbc308d8209dbf1a%7Cafb58802ff7a4bb1ab21367ff2ecfc8b%7C0%7C0%7C637295209184273315&sdata=PbscIaF1YgoA6TOFydENsrn79iERjXLdAeV9g7b5u94%3D&reserved=0>
>
> under section on "Verification of correctness”, there is this statement
>
> *(e.g., for linear elements, do not use the QGauss(2) quadrature formula)*
>
> because solution may exhibit superconvergence at the QGauss(2) points.
>
> If we solve
>
> -u’’ = 16*pi^2*sin(4*pi*x) in (0,1)
> u(0) = 0, u(1) = 1
>
> using 8 linear elements and QGauss(2) for quadrature.
>
> The error is very small at the vertices of the mesh, not at the QGauss(2) points.
>
> Can you look into this issue, is the comment in the documentation wrong,
> perhaps it should say *do not use QGaussLobatto(2)* ? Or is there some issue I
> am missing here ?
Ah, very interesting question! You're right that in some situations -- the
Laplace equation in 1d specifically -- the superconvergence points are in fact
the vertices of the cells.
But that's not true in 2d/3d. There, at least the recollection I have from
when I learned about this many years ago, the superconvergence points are
indeed the Gauss points. Want to try that out as well in a small experiment?
Say take a 16x16 mesh, and plot both solution and discrete solution in a part
of the domain well away from the boundary, and see where the two seem to
intersect.
(As always, we're always happy to improve the documentation. Clearly, what I
said in step-7 is not the complete truth and ought to be improved, but I'd
rather we check what we say before coming up with a better description :-) )
Cheers
W.
--
------------------------------------------------------------------------
Wolfgang Bangerth email:
bang...@colostate.edu
www:
http://www.math.colostate.edu/~bangerth/