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s_grad_grad(3rheolef) rheolef-6.1 s_grad_grad(3rheolef)

NAME

s_grad_grad -- grad_grad-like operator for the Stokes stream function computation

SYNOPSIS

      form(const space V, const space& V, "s_grad_grad");
 

DESCRIPTION

Assembly the form associated to the -div(grad) variant operator on a finite element space V. The V space may be a either P1 or P2 finite element space. See also form(2) and space(2). On cartesian coordinate systems, the form coincide with the "grad_grad" one (see grad_grad(3)):
 
               /
               |
      a(u,v) = |  grad(u).grad(v) dx
               |
               / Omega
 
The stream function on tri-dimensionnal cartesian coordinate systems is such that
 
       u = curl psi
       div psi = 0
 
where u is the velocity field. Taking the curl of the first relation, using the identity:
 
        curl(curl(psi)) = -div(grad(psi)) + grad(div(psi))
 
and using the div(psi)=0 relation leads to:
 
        -div(grad(psi)) = curl(u)
 
This relation leads to a variational formulation involving the the "grad_grad" and the "curl" forms (see grad_grad(3), curl(3)).
In the axisymmetric case, the stream function psi is scalar ans is defined from the velocity field u=(ur,uz) by (see Batchelor, 6th ed., 1967, p 543):
 
                 d psi                       d psi
      uz = (1/r) -----    and   ur = - (1/r) -----
                  d r                         d r
 
See also http://en.wikipedia.org/wiki/Stokes_stream_function . Multiplying by rot(xi)=(d xi/dr, -d xi/dz), and integrating with r dr dz, we get a well-posed variationnal problem:
 
        a(psi,xi) = b(xi,u)
 
with
 
                  /
                  | (d psi d xi   d psi d xi)
      a(psi,xi) = | (----- ---- + ----- ----) dr dz
                  | ( d r  d r     d z  d z )
                  / Omega
 
and
 
                /
                | (d xi      d xi   )
      b(xi,u) = | (---- ur - ---- uz) r dr dz
                | (d z       d r    )
                / Omega
 
Notice that a is symmetric definite positive, but without the 'r' weight as is is usual for axisymmetric standard forms. The b form is named "s_curl", for the Stokes curl variant of the "curl" operator (see s_curl(3)) as it is closely related to the "curl" operator, but differs by the r and 1/r factors, as:
 
                   (       d (r xi)     d xi )
        curl(xi) = ( (1/r) -------- ; - -----)
                   (         d r        d z  )
 
while
 
                   ( d xi       d xi )
      s_curl(xi) = ( ----  ;  - ---- )
                   ( d r        d z  )
 

EXAMPLE

The following piece of code build the form associated to the P1 approximation:
 
        geo g("square");
        space V(g, "P1");
        form a(V, V, "s_grad_grad");
 
 
 
 

SEE ALSO

form(2), space(2), grad_grad(3), grad_grad(3), curl(3), s_curl(3)
rheolef-6.1 rheolef-6.1