I took a look at your (incomplete) step-58, which (as far as I could 
understand) solves the equation, but without propagating it in space, just 
in time. I would like to propagate the result in time and accordingly in 
space, i.e. if the pulse propagates through a fiber, I would like to see 
the moving pulse. Is that possible?
The matrix I was mentioning earlier would be a dense matrix, formed 
according to the DHT-method (i.e. no relation to FEM)

Am Dienstag, 23. Juli 2019 22:35:57 UTC+2 schrieb Wolfgang Bangerth:
>
> On 7/22/19 1:32 AM, 'Maxi Miller' via deal.II User Group wrote: 
> > More or less, yes, together with how I could get the "column" vector I 
> would 
> > like to apply the matrix to. It is not a problem to do that in a 
> FTDT-setting, 
> > but I do not know how to do that in a FEM-setting. 
>
> When you say "column vector", you mean the vector of unknowns that 
> corresponds 
> to one column of nodes in the mesh? 
>
Yes, basically 

>
> One can think of deal.II Triangulations as unstructured meshes. So 
> extracting 
> a column of nodes is not a natural thing to do. But you can of course 
> always 
> loop over all nodes (e.g., using DoFTools::map_dofs_to_support_points()) 
> and 
> group them by the x-coordinate of their location. 
>
> How you would build this matrix? That's something we can't know without 
> actually seeing a formula for the operator you're thinking of. 
>
> Best 
>   W. 
>
> -- 
> ------------------------------------------------------------------------ 
> Wolfgang Bangerth          email:                 bang...@colostate.edu 
> <javascript:> 
>                             www: http://www.math.colostate.edu/~bangerth/ 
>
>

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