 
  
  
  
  
 
We have implemented a sophisticated incompressible flow solver using DIME and DIMEFEM. The algorithm is described more completely in [Bristeau:87a]. The evolution equation for an incompressible Newtonian fluid of viscosity n is

We use a three-stage operator-split scheme whereby for each time step of length dt, the equation is integrated
 with incompressibility and no convection,
then
 with incompressibility and no convection,
then
 to
 to  with convection and 
no incompressibility condition, then
 with convection and 
no incompressibility condition, then 
The parameter  is
 is  .
.
Each of these three implicit steps involves the solution of either a Stokes problem:

or the nonlinear problem:\

where  is a parameter inversely proportional to the time step.  We 
solve the Navier-Stokes equation,  and
consequently also these subsidiary problems, with given velocity at the
boundary (Dirichlet boundary conditions).
 is a parameter inversely proportional to the time step.  We 
solve the Navier-Stokes equation,  and
consequently also these subsidiary problems, with given velocity at the
boundary (Dirichlet boundary conditions).