It certainly won't be that simple. You'll need to look through the
literature to figure it out. I suspect it will require re-introducing
a pressure into the equations and then transforming the continuity
equation into an equation for pressure.
On Thu, Oct 11, 2018 at 4:06 AM fgendr01 wrote:
>
> Th
Thanks Daniel for your answer,
I used the continuity equation (nabla vector velocity) to obtain the equation
in temperature.
But actually, maybe we should use it as a constraint to my problem.
But now, how can I create this constraint ? with a new equation ?
I tried : velocity.divergence == 0 but
Don't you still have a $\nabla . \vec{u} = 0$ equation though? It
doesn't go away. That equation becomes like a constraint.
https://www.comsol.com/multiphysics/boussinesq-approximation
On Wed, Oct 10, 2018 at 5:58 AM fgendr01 wrote:
>
> Hi Daniel,
> Thank you for your answer.
> I thank you for t
Hi Fabien,
I looked over your problem and I haven't been able to debug it. I
tried various combinations of constraints and I'm not sure why it's
becoming nonphysical (dT >1 or dT < -1). It would require getting into
the code and looking at the numbers in the offending cells.
One thing that worrie
Fabien -
I don't know where the problem lies, but my recommendation would be to
systematically take the problem back toward the code I previously gave you.
While that code didn't produce the image you were looking for, the behavior
seemed consistent and it wasn't unstable.
As far as I can tell
Yes I tried without kinematic boundary conditions and there is no difference !
Maybe the scheme is not stable.
Other ideas ?
Fabien
> Le 17 sept. 2018 à 22:27, Thibault Bridel-Bertomeu
> a écrit :
>
> Have you tried without the kinematic boundary conditions ? Just constrain T
> and dT/dn, wha
Hi again Fabien,
Well, I would say that physically it makes sense. With such boundary
condition, I think the problem is well posed. Now it is all about the
numerics.
Have you tried ? What does the solver yield ?
Cheers
Thibault
Le lun. 17 sept. 2018 à 21:49, fgendr01 a
écrit :
> Thanks Thibault
Thanks Thibault,
You’re right, the top ans the bottom walls are adiabatic and I tried to put
velocity conditions.
What do you think about these conditions :
# Boundary Conditions
T.constrain(Tmax, mesh.facesLeft)
T.constrain(Tmin, mesh.facesRight)
T.faceGrad.constrain(0, mesh.facesTop)
T.faceGrad
Thanks a lot Jon.
I appreciate your help.
I will try to apply your remarks but I will certainly still need your help
again ;-) to develop the code.
Thanks again.
Fabien
> Le 15 août 2018 à 19:46, Guyer, Jonathan E. Dr. (Fed)
> a écrit :
>
> Fabien -
>
> I think the code below should get you
Fabien -
I think the code below should get you going.
The changes I made were:
- `xVelocity` and `zVelocity` changed to rank-0 CellVariables. FiPy *always*
solves at cell centers.
- Created a rank-1 FaceVariable to hold the velocity. The cell components must
be interpolated and manually insert
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