Wikipedia / Weak formulation
Wikipedia / Weak formulation
Weak formulations are tools for the analysis of mathematical equations that permit the transfer of concepts of linear algebra to solve problems in other fields such as partial differential equations. In a weak formulation, equations or conditions are no longer required to hold absolutely (and this is not even well defined) and has instead weak solutions only with respect to certain "test vectors" or "test functions". In a strong formulation, the solution space is constructed such that these equations or conditions are already fulfilled.
The Lax–Milgram theorem, named after Peter Lax and Arthur Milgram who proved it in 1954, provides weak formulations for certain systems on Hilbert spaces.
General concept
be a Banach space be the dual space be a linear map is a solution of the equation
,
is called a test vector (in general) or a test function is a function space).
such that
by defining the bilinear form
Example 1: linear system of equations
be a linear mapping. Then, the weak formulation of the equation
the following equation holds:
denotes an inner product.
Since the inner product is bilinear, it is sufficient to test with basis vectors, and we get
Actually, expanding we obtain the matrix form of the equation
and
The bilinear form associated to this weak formulation is
Example 2: Poisson's equation
To solve Poisson's equation
on its boundary later, one can use the scalar product
to derive the weak formulation. Then, testing with differentiable functions yields
The left side of this equation can be made more symmetric by integration by parts using Green's identity on
This is what is usually called the weak formulation of Poisson's equation. Functions must be zero on the boundary, and have square-integrable derivatives. The appropriate space to satisfy these requirements is the Sobolev space of functions with weak derivatives and with zero boundary conditions, so
The generic form is obtained by assigning
and
The Lax–Milgram theorem
This is a formulation of the Lax–Milgram theorem which relies on properties of the symmetric part of the bilinear form. It is not the most general form.
be a real Hilbert space a bilinear form on which is
Then, for any bounded to the equation
and it holds
Application to example 1
Here, application of the Lax–Milgram theorem is a stronger result than is needed.
Coercivity: this actually means that the real parts of the eigenvalues. Since this implies in particular that no eigenvalue is zero, the system is solvable.
is the minimal real part of an eigenvalue of
Application to example 2
where the norm on the right is the by the Poincaré inequality and by the Cauchy–Schwarz inequality,
Therefore, for any of Poisson's equation and we have the estimate
See also
References
External links