Stokes operator
The Stokes operator, named after George Gabriel Stokes, is an unbounded linear operator used in the theory of partial differential equations, specifically in the fields of fluid dynamics and electromagnetics.
Definition
If we define 
 as the Leray projection onto divergence free vector fields, then the Stokes Operator 
 is defined by
where 
 is the Laplacian.  Since 
 is unbounded, we must also give its domain of definition, which is defined as 
, where 
.  Here, 
 is a bounded open set in 
 (usually n = 2 or 3), 
 and 
 are the standard Sobolev spaces, and the divergence of 
 is taken in the distribution sense.
Properties
For a given domain 
 which is open, bounded, and has 
 boundary, the Stokes operator 
 is a self-adjoint positive-definite operator with respect to the 
 inner product.  It has an orthonormal basis of eigenfunctions 
 corresponding to eigenvalues 
 which satisfy
and 
 as 
.  Note that the smallest eigenvalue is unique and non-zero.  These properties allow one to define powers of the Stokes operator.  Let 
 be a real number.  We define 
 by its action on 
:
where 
 and 
 is the 
 inner product.
The inverse 
 of the Stokes operator is a bounded, compact, self-adjoint operator in the space 
, where 
 is the trace operator.  Furthermore, 
 is injective.
References
- Temam, Roger (2001), Navier-Stokes Equations: Theory and Numerical Analysis, AMS Chelsea Publishing, ISBN 0-8218-2737-5
 - Constantin, Peter and Foias, Ciprian. Navier-Stokes Equations, University of Chicago Press, (1988)
 


