[Insight-users] FEM: PDE of Crank-Nicolson solver
brian avants
stnava at gmail.com
Wed Dec 15 11:04:32 EST 2010
Cristina
Thanks for the reminder about what's written there --- it clearly
should be updated. Some additional definitions:
M --- the mass matrix ( covered in any basic FEM book or webpage ).
rho --- this is a scalar that determines the "density" of the mass matrix.
U --- the deformation field.
t --- time.
K --- the stiffness matrix.
alpha --- in crank-nicolson, set to 0.5 , but often used with 0 or 1.
A generic PDE this would solve would read something like:
$ \rho \partial U / \partial t + L U = f $
where \rho and L are determined by the physics of the problem. What
I am confused about is this part:
dt*(\alpha*f_{n+1} + (1-\alpha)*f_n)
The n should probably be replaced with t indices that are similar to
those accumulating the U solution. The code seems to verify this:
void SolverCrankNicolson::RecomputeForceVector(unsigned int index)
{//
Float ft = m_ls->GetVectorValue(index,ForceTIndex);
Float ftm1 = m_ls->GetVectorValue(index,ForceTMinus1Index);
Float utm1 = m_ls->GetVectorValue(index,DiffMatrixBySolutionTMinus1Index);
Float f=m_deltaT*(m_alpha*ft+(1.-m_alpha)*ftm1)+utm1;
m_ls->SetVectorValue(index , f, ForceTIndex);
}
If I find a reference that shows this particular discretization, I
will share it. However, this approach solves a common static problem
if alpha = 1 and if f is static. You can verify this yourself.
Brian
> " * FEM Solver for time dependent problems; uses Crank-Nicolson implicit
> discretization scheme.
> *It solves the following problem:
> *
> * ( M + alpha*dt* K )*U_t=(M - (1.- alpha)*dt* K)* U_{t-1} +
> dt*(alpha*f_{n+1} + (1-alpha)*f_n) "
M is the element's mass matrix
>
> This problem formulation differs from the one obtained for the heat equation
> (for example). So, I guess that it comes from an specific PDE by applying
> Crank-Nicolson discretization scheme to it. My questions then are:
> 1. From which PDE does it come from? Which one is the problem that it is
> trying to solve?
> 2. If the PDE is different depending on the element that one chooses, should
> not one get different problem formulations to solve by choosing different
> elements (PDE)? And then is it the solver generic or valid for only one PDE?
>
> Thank you!
>
> Cristina
>
> On Fri, Dec 10, 2010 at 8:59 PM, brian avants <stnava at gmail.com> wrote:
>>
>> Hi Cristina
>>
>> The specific PDE depends upon the specific elements you choose. For
>> instance, if you set up a triangular mesh via the
>> 2DC0LinearTriangularMembrane element, then you will use a membrane
>> energy penalty term.
>>
>> The Crank-Nicolson solver uses the Crank-Nicolson approach to
>> accumulate the solution to the registration problem over time.
>>
>> Wikipedia provides a reasonable general explanation of the C-N
>> approach and gives an example for the heat equation;
>>
>> http://en.wikipedia.org/wiki/Crank%E2%80%93Nicolson_method
>>
>> B.
>>
>>
>> On Fri, Dec 10, 2010 at 10:07 AM, Cristina Oyarzun
>> <coyarzunlaura at googlemail.com> wrote:
>> > Hello,
>> >
>> > I am using itk FEM registration filter. This filter makes use of
>> > itkFEMSolverCrankNicolson. In the header file of the solver one finds
>> > the
>> > equation that the solver tries to solve. However, one can only find
>> > there
>> > its Crank-Nicolson formulation but not the original PDE that leads to
>> > that
>> > equation.
>> >
>> > I tried to get the discretized equation by using the equation of motion
>> > that
>> > is described in a book and Crank-Nicolson scheme but did not arrive to
>> > the
>> > same solution. Could someone tell me which on is the original PDE that
>> > is
>> > solved in itkFEMSolverCrankNicolson?
>> >
>> > Thank you!!
>> >
>> > Greetings,
>> >
>> > Cristina
>> >
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>
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