From 21629558d3603d7f2401f8ce7f5266c08aee2dad Mon Sep 17 00:00:00 2001 From: schrage Date: Tue, 23 Mar 1999 15:04:09 +0000 Subject: [PATCH] Added chapter 0: FE program structure. git-svn-id: https://svn.dealii.org/trunk@1036 0785d39b-7218-0410-832d-ea1e28bc413d --- deal.II/doc/tutorial/index.html | 40 +++++++++++++++++++-------------- 1 file changed, 23 insertions(+), 17 deletions(-) diff --git a/deal.II/doc/tutorial/index.html b/deal.II/doc/tutorial/index.html index 513405feab..f51da81086 100644 --- a/deal.II/doc/tutorial/index.html +++ b/deal.II/doc/tutorial/index.html @@ -2,15 +2,15 @@ "http://www.w3.org/TR/REC-html40/strict.dtd"> - - The DEAL Tutorial + + The deal.II Tutorial - + -

The DEAL Tutorial

+

The deal.II Tutorial

-

or DEAL in several easy and some more hard lessons

+

or deal.II in several easy and some more hard lessons

Prerequisites

@@ -29,30 +29,36 @@

This tutorial is split into several parts, starting with the stationary Laplace problem and advancing to more complicated problems. If you have never - used DEAL we recommend that you begin at the beginning and + used deal.II we recommend that you begin at the beginning and advance through the chapters in their proper order. This tutorial contains the complete code for every example program and can be used as a reference, too, if you are looking for code to solve a specific problem with - DEAL. + deal.II.

-

On DEAL

+

On deal.II

- DEAL is short for Differential Equations Analysis Library, + deal.II is short for Differential Equations Analysis Library, version II, which says it all, really. Its purpose it the solution of partial differential equations on unstructured grids with error control. You can find more - information on DEAL and some examples at - - http://gaia.iwr.uni-heidelberg.de/DEAL/. DEAL was written + information on deal.II and some examples at + + http://gaia.iwr.uni-heidelberg.de/~deal/. deal.II was written by the numerics group at the IWR, University of Heidelberg.

+

Chapter 0: Structure of a + Finite Element Program

+

We will discuss the various elements needed for a working + finite element program and some of the possibilitier + deal.II offers in this respect. +

Chapter 1: The Laplace - problem

+ Problem

- We will solve the stationary Laplace problem on a square grid with zero - boundary condition on three of the edges and a constant boundary condition on - one edge. + We will solve the stationary Laplace problem on a square grid with + boundary conditions of the form cos(2*PI*x)cos(2*PI*y). + You can also obtain the source code.

Technical terms

@@ -65,7 +71,7 @@
Jan Schrage

- Last modified: Tue 5 Jan 1999 + Last modified: Tue 9 Mar 1999

-- 2.39.5