Hi all,
The attached pdf might be useful. There is some notational difference from
step44, but it is defined here.
Thanks,
Anup
On Wed, Nov 9, 2016 at 12:41 PM, Andrew McBride
wrote:
> Dear Claire
>
> You might also be interested in the one-field version of step-44 in the
> code gallery https:
Dear Claire
You might also be interested in the one-field version of step-44 in the code
gallery
https://dealii.org/developer/doxygen/deal.II/code_gallery_Quasi_static_Finite_strain_Compressible_Elasticity.html
A
> On 9 Nov 2016, at 18:24, Claire wrote:
>
> Dear Wolfgang and Jean-Paul,
>
Dear Wolfgang and Jean-Paul,
I will try to do my best to produce the document and give a contribution
(even small) to the library.
I am not sure when exactly I will be able to have time to make it though...
The problem that I personally try to solve is simpler and does not require
a three field
On 11/08/2016 01:36 AM, Jean-Paul Pelteret wrote:
You're welcome. If you go through the formulation and still don't have full
clarity, then let me know. I do have this derivation documented somewhere...
Claire -- If, on the other hand, you do figure it out, write it up into a
one-page latex d
Dear Claire,
You're welcome. If you go through the formulation and still don't have full
clarity, then let me know. I do have this derivation documented somewhere...
Regards,
Jean-Paul
On Tuesday, November 8, 2016 at 9:29:23 AM UTC+1, Claire wrote:
>
> Dear Jean-Paul,
>
> Thank you very much fo
Dear Jean-Paul,
Thank you very much for your answer.
I still have to figure out some of the calculations you suggested me to do,
but I got the concepts and the reason why the gradients are defined on the
deformed configuration rather than on the initial one.
Best,
Claire
Le lundi 7 novembre
Dear Claire,
You are right that this is a total Lagrangian formulation but that doesn't
mean that one is restricted to defining the problem in terms of fully
referential quantities.
One can arrive at the same conclusion from a number of starting points, but
ultimately its because we'd chosen
