From 5b291e61c715ebff89b0b35b645363416fc988ae Mon Sep 17 00:00:00 2001 From: Wolfgang Bangerth Date: Thu, 21 Feb 2013 20:12:44 +0000 Subject: [PATCH] Make notation consistent with the way we discuss this in the video lecture on the topic. git-svn-id: https://svn.dealii.org/trunk@28516 0785d39b-7218-0410-832d-ea1e28bc413d --- deal.II/examples/step-20/step-20.cc | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/deal.II/examples/step-20/step-20.cc b/deal.II/examples/step-20/step-20.cc index bbe7752348..2e44d3b44c 100644 --- a/deal.II/examples/step-20/step-20.cc +++ b/deal.II/examples/step-20/step-20.cc @@ -685,7 +685,7 @@ namespace Step20 Vector tmp (solution.block(0).size()); - // Now on to the first equation. The right hand side of it is BM^{-1}F-G, + // Now on to the first equation. The right hand side of it is $B^TM^{-1}F-G$, // which is what we compute in the first few lines. We then declare the // objects representing the Schur complement, its approximation, and the // inverse of the approximation. Finally, we declare a solver object and @@ -725,7 +725,7 @@ namespace Step20 } // After we have the pressure, we can compute the velocity. The equation - // reads MU=-B^TP+F, and we solve it by first computing the right hand + // reads $MU=-BP+F$, and we solve it by first computing the right hand // side, and then multiplying it with the object that represents the // inverse of the mass matrix: { -- 2.39.5