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May 23, 2012, 06:13 |
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#101 |
Senior Member
Anton Kidess
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Would there be a difference for laminar flow? All we need in the boundary condition is the face normal, which is available for a basic patch. I think the wall-BC is only needed for the turbulence models.
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May 23, 2012, 06:39 |
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#102 |
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Andrea Ferrari
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i do not understand what you mean, poiseuille flow is something expected even for laminar flow for ex.
i said that i would choose fixedValue uniform(0 0 0) for the lateral area of the cylinder and fixedValue uniform(0 0 0.001) for inlet and outlet. These are in my opinion the correct (physical) boundary condition for a liquid that moves in a capillary tube. Now the paper is talking about uniform velocity field, so using these BC you will have parabolic profile, at least far from the droplet (not uniform). I do not understand the need of capillary tube, would be more clear for me if the drop moves simply in another liquid with fixed velocity everywhere. btw the BC you choose are: zeroGaradient for pressure everywhere fixedValue for U (0 0 0.001) everywhere right? andrea |
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May 23, 2012, 08:39 |
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#103 |
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Anton Kidess
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Sorry, I totally misunderstood your initial question! You are right that for a real capillary tube, there should be a no-slip on the walls and we'd have a parabolic flow profile if the flow is assumed developed. However, that would introduce shear on the droplet, and they don't want that in this test case. So in the end it is just a droplet with no relative motion to a flowing surrounding liquid. Why they went to the trouble making a cylindric domain instead of a plain box might just be to cut away some cells in the domain which are unnecessary to maintain a minimum distance to the walls.
- Anton
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May 24, 2012, 06:35 |
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#104 |
Senior Member
Andrea Ferrari
Join Date: Dec 2010
Posts: 319
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Hi,
my simulation is really bad. the drop starts to move along the z-axis but then, after a while, it diffuses away and the maximum value of alpha goes to 0.6/0.5. How are your results? andrea |
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May 24, 2012, 08:58 |
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#105 |
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Anton Kidess
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Andrea, unfortunately I don't have results yet. I'm busy with other things so I don't have much time to play with interFoamSSF these days. I'll report back once I have something. Good luck!
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May 30, 2012, 09:02 |
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#106 |
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Anton Kidess
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I pushed updates to enable the use of adjustable time stepping.
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May 31, 2012, 08:41 |
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#107 |
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Anton Kidess
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I now have results on the moving droplet case with the SSF and CSF formulations - see attachment. As expected, they are both not great.
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May 31, 2012, 08:53 |
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#108 |
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Andrea Ferrari
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Hi Anton,
can you upload the test case with boundary and initial conditions on the repository. just to be sure we are using the same. thanks andrea |
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May 31, 2012, 09:21 |
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#109 |
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Anton Kidess
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Ok, I uploaded the case. What I did was initialize the droplet shape starting from a square droplet of same volume, and then (after 0.0005s) turn on the background velocity field and start doing the real simulation.
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June 1, 2012, 05:13 |
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#110 |
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Anton Kidess
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I noticed something about the Crank-Nicholson scheme - the programmers guide on page 43 states you have to implement a mixing of fvm and fvc terms manually! Is that really up to date, i.e. is it really not enough to modify fvSchemes?
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June 2, 2012, 10:50 |
reducing paracurr on unstructured grids
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#111 |
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Jake
Join Date: May 2012
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Hi guys,
first off its been really interesting to follow your conversation and to see your progress. I've just started off working on reducing parasitic currents and i was wondering if you have any results or approaches/ideas to reduce these on unstructured grids. Thx Jakob |
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June 3, 2012, 13:18 |
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#112 |
Senior Member
Andrea Ferrari
Join Date: Dec 2010
Posts: 319
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@Anton
good question. i've never used crank nicholson scheme for my simulations and so i really do not known. My first guess is that it is enough to modify fvScheme but i am not sure. @Jakob Did you try the drop relaxation on unstructured grid? it would be a good starting point. best |
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June 4, 2012, 06:08 |
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#113 |
Senior Member
Andrea Ferrari
Join Date: Dec 2010
Posts: 319
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I tried to add changes to use adjustable time step but i got some errors about pimple control. I copied pimpleControl.H/C/I.H from openFoam 2.0.1 in interFoamSSF's folders. This is the error
interFoam.C:215: error: ‘class Foam:impleControl’ has no member named ‘nCorrPISO’ In file included from interFoam.C:217: pEqn.H:54: error: no matching function for call to ‘Foam:impleControl::finalInnerIter()’ pimpleControlI.H:100: note: candidates are: bool Foam:impleControl::finalInnerIter(Foam::label, Foam::label) const interFoam.C:100: warning: unused variable ‘cycle’ /home/aferrari/OpenFOAM/OpenFOAM-2.1.0/src/finiteVolume/lnInclude/readTimeControls.H:38: warning: unused variable ‘maxDeltaT’ make: *** [Make/linux64GccDPOpt/interFoam.o] Error 1 i think nCorrPISO has to be changed with nOuterCorr, right? but i don't know what to do with the other error. any suggests? best andrea |
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June 4, 2012, 06:23 |
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#114 |
Senior Member
Andrea Ferrari
Join Date: Dec 2010
Posts: 319
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ok i solved it. (nCorrPiso is nCorr and in pEqn:h i changed pEqn.solve to match your version). would be great to have the full version compiled with OF 2.1.0.
best |
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June 4, 2012, 07:01 |
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#115 | |
Senior Member
Anton Kidess
Join Date: May 2009
Location: Germany
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Quote:
Code:
* Start with Roberto's version for OpenFoam 2.1 (http://code.google.com/r/robertocastillalopez-interfoamssf-210) * hg pull from my repository (http://code.google.com/p/interfoamssf) in the interfoamssf-210 folder to get my updates * Run 'hg merge' to combine the two versions into one * Run 'hg commit' to store the merge changes for the future Good guides on using mercurial are http://hgbook.red-bean.com/read/ or http://hginit.com.
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June 4, 2012, 07:17 |
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#116 | |
Senior Member
Anton Kidess
Join Date: May 2009
Location: Germany
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Quote:
Cheers, Anton
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June 6, 2012, 07:43 |
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#117 |
Senior Member
Andrea Ferrari
Join Date: Dec 2010
Posts: 319
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Hi Anton,
my simulation is still bad, it is loosing mass. The maximum value of alpha1 drops down to 0.5 after few time steps. Any idea of why?. Do you see the same? best andrea |
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June 7, 2012, 08:35 |
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#118 |
Senior Member
Anton Kidess
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In my case the droplet retains it's shape and position until 0.005s (100 time steps), after which it moves off-center and starts diffusing away completely (at this point the volume fraction field isn't conserved any more).
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June 7, 2012, 08:55 |
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#119 |
Senior Member
Andrea Ferrari
Join Date: Dec 2010
Posts: 319
Rep Power: 17 |
i observed exactly the same behavior. I hope this is due to lack of the filtering step. i'll start to think about the implementation as soon i'll have time.
best andrea |
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June 11, 2012, 09:37 |
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#120 |
Senior Member
Anton Kidess
Join Date: May 2009
Location: Germany
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I started working on the filtering, and I stumbled across an issue with it's formulation. Have a look at the attached image - let's say it's an interface with a slight curvature. 'deltasf' is computed at the faces and will be large in normal to the interface (y) and small in tangential direction (x). Keeping that in mind for equation (22) of the paper, that means we would start filtering in y-direction instead of x. Right?
Further issues: The value of epsilon is undefined, and it is unclear when to apply eq (23)...
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Tags |
capillary flows, interfoam, parasitic currents |
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