FEM2D_NAVIER_STOKES_INOUT
"Inout" Routines for FEM2D_NAVIER_STOKES


FEM2D_NAVIER_STOKES_INOUT is a FORTRAN90 library which supplies information defining a Navier-Stokes flow problem in the "inout" region, which is a square region that is 1 unit wide and 1 unit high. A parabolic inflow is specified on the lower left, and a zero Neumann outflow is specified on the upper right.

The Neumann condition on the outflow is not working as expected, so we have temporarily backtracked to using a Dirichlet outflow condition there...

To run the problem directly, you only need the user-supplied routines in inout.f90, the node data in nodes6.txt, and the element data in triangles6.txt.

You compile and link the solver with inout.f90, using commands like:

        gfortran fem2d_navier_stokes.f90 inout.f90
        mv a.out channel
      
and then run the program with the command
        ./inout nodes6.txt triangles6.txt
      

Licensing:

The computer code and data files described and made available on this web page are distributed under the GNU LGPL license.

Languages:

FEM2D_NAVIER_STOKES_INOUT is available in a FORTRAN90 version.

Related Data and Programs:

FEM2D_NAVIER_STOKES, a FORTRAN90 program which solves the 2D incompressible Navier-Stokes equations in an arbitrary triangulated region. In order to run, it requires user-supplied routines that define problem data.

FEM2D_NAVIER_STOKES_CAVITY, a FORTRAN90 library which contains the user-supplied routines necessary to run fem2d_navier_stokes on the "cavity" problem.

FEM2D_NAVIER_STOKES_CHANNEL, a FORTRAN90 library which contains the user-supplied routines necessary to run fem2d_navier_stokes on the "channel" problem.

Source Code:

The geometry is defined by sets of nodes and triangles. The velocities use the full set of nodes, and quadratic (6 node) triangles.

The pressures are associated with a subset of the nodes called "pressure nodes", and linear (3 node) triangles. Note that, in the order 3 triangulation, the nodes are renumbered, and do NOT inherit the labels used in the order 6 triangulation.

The nonlinear Navier Stokes equations are solved, using the Stokes solution as a starting point.


Last revised on 28 December 2010.