Updated the documentation to make clear that we are solving -Delta u = 1
with u = 0 on the boundary.
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@ -10,14 +10,15 @@
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To see options: ex10 -help
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Description: This code solves a system corresponding to a discretization
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of the Laplace equation with zero boundary conditions on the
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unit square. The domain is split into a n x n grid of
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quadrilateral elements and each processors owns a horizontal
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strip of size m x n, where m = n/nprocs. We use bilinear
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finite element discretization, so there are nodes (vertices)
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that are shared between neighboring processors. The Finite
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Element Interface is used to assemble the matrix and solve
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the problem. Nine different solvers are available.
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of the Laplace equation -Delta u = 1 with zero boundary
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conditions on the unit square. The domain is split into
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a n x n grid of quadrilateral elements and each processors
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owns a horizontal strip of size m x n, where m = n/nprocs. We
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use bilinear finite element discretization, so there are
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nodes (vertices) that are shared between neighboring
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processors. The Finite Element Interface is used to assemble
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the matrix and solve the problem. Nine different solvers are
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available.
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*/
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#include <math.h>
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@ -10,15 +10,16 @@
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To see options: ex3 -help
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Description: This code solves a system corresponding to a discretization
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of the Laplace equation with zero boundary conditions on the
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unit square. The domain is split into an N x N processor grid.
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Thus, the given number of processors should be a perfect square.
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Each processor's piece of the grid has n x n cells with n x n
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nodes connected by the standard 5-point stencil. Note that the
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struct interface assumes a cell-centered grid, and, therefore,
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the nodes are not shared. This example demonstrates more
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features than the previous two struct examples (Example 1 and
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Example 2). Two solvers are available.
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of the Laplace equation -Delta u = 1 with zero boundary
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conditions on the unit square. The domain is split into
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an N x N processor grid. Thus, the given number of processors
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should be a perfect square. Each processor's piece of the
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grid has n x n cells with n x n nodes connected by the
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standard 5-point stencil. Note that the struct interface
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assumes a cell-centered grid, and, therefore, the nodes are
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not shared. This example demonstrates more features than the
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previous two struct examples (Example 1 and Example 2). Two
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solvers are available.
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To incorporate the boundary conditions, we do the following:
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Let x_i and x_b be the interior and boundary parts of the
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