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- - **Moving mesh problem OpenFoam 141**
(*https://www.cfd-online.com/Forums/openfoam-solving/57916-moving-mesh-problem-openfoam-141-a.html*)

Hello everybody
Context: I'Hello everybody
Context: I'm coupling a FEM code (Feap) and OpenFOAM to solve FSI problems by a partitionned strategy. I try to validate this coupling. To be more precise, i'm using the solver icoDyMFoam of OpenFOAM 1.4.1. The mesh is solved with the following options : // ---------- dynamicMeshDict --------- dynamicFvMesh dynamicMotionSolverFvMesh; motionSolverLibs ("libfvMotionSolvers.so"); solver velocityLaplacian; diffusivity quadratic inverseDistance 1(movingWall); // -------------------------------------------------- As from other post and sources [1] it seems that the quadratic inverse give the best results. Unfortunately, when the motions become to big (for problem with a small stiffness), it seems the computation crash due to bad motion (see pictures [2]) of the mesh that become non-convex. Is this for you due to bad mesh construction, bad options to solve the mesh motions or any other idea ? Thank you. [1] Automatic Mesh Motion for the Unstructured Finite Volume Method by Hrvoje Jasak and Zeljko Tukovic [2] Pictures velocity field: <https://perso.crans.org/kassiotis/op...velocity74.jpg> initial mesh: <https://perso.crans.org/kassiotis/openfoam/mesh0.jpg> deformed mesh with problem: <https://perso.crans.org/kassiotis/openfoam/mesh74.jpg> |

Hello,
For this sort of motHello,
For this sort of motion you really need to use a vertex-based mesh motion techniques rather than the FV motion you have chose. Vertex-based motion described in my/our paper is available in the SVN version of OpenFOAM - the Forum will show you how to get it. In terms of motion, we have done MUCH more severe cases than yours with reasonable success. Examples are in some of my presentations, available on: http://powerlab.fsb.hr/ped/kturbo/OpenFOAM/slides/ You can also find a series of moving mesh movies in: http://powerlab.fsb.hr/ped/kturbo/OpenFOAM/movies/ Example most similar to yours is an oscillating NACA airfoil with a sharp trailing edge: Oscillating NACA airfoil - FEM mesh motion Specification of mesh motion I use is typically something like this: twoDMotion yes; solver laplaceFaceDecomposition; diffusivity quadratic; frozenDiffusion off; distancePatches ( oldInternalFaces ); In your case, 2-D motion should be set to yes. Please have a go and tell me more about problems you encounter. Enjoy, Hrv |

When large rotations come intoWhen large rotations come into play, I have very good experience with the displacement Solid Body Rotation fvMotionSolver.......
Hrv, why do you suggest a vertex-based technique for this kind of motion??? Frank |

Hrv, why do you suggest a veQuote:
Hrv |

Referring to your tetDecomp stReferring to your tetDecomp stuff, it is a very nice method and very robust. Unfortunately, I need some rotational motion solvers (like the SBR Stress model) which is not implemented for your tetDecomp solvers.
So, Christophe, I would say, just play with all motion solvers (tetDecomp, displacement FV and velocity FV) to find which one is best suited for your problem. Frank |

Hello Hrv,
A Good day to yoHello Hrv,
A Good day to you! Been a while since my last post :-)! Though... have been keeping my eyes open on everything that has been going on here! I had a short question, and it would be great if you could shed some light (as usual).... Could you tell me something about the Deformation Energy and Distortion Energy motion diffusivity options you have implemented in the vertex based motion solvers ? Under what situations would you use these diffusivity methods, and what are the advantages and disadvantages compared to the other methods? Also, what would a good value be for the exponent in each case? (Or even better... how could one decide on a good value?) Have a nice evening! Philippose |

A lovely paper for you:
@A lovely paper for you:
@Article{Jasak:MeshMotion, author = {Jasak, H. and Tukovic, Z., title = {Automatic Mesh Motion for the Unstructured Finite Volume Method}, journal = {Transactions of FAMENA}, year = 2007, volume = 30, number = 2, pages = {1-18} }} http://powerlab.fsb.hr/ped/kturbo/Op...tionFAMENA.pdf It's all explained there (by Zeljko) with examples, definitions etc. and all in English http://www.cfd-online.com/OpenFOAM_D...part/happy.gif Enjoy, Hrv P.S. Please refer to paper where appropriate - Zeljko needs all the exposure he can get for the wonderful work he did for his PhD and since. |

Hi again,
Thanks a lot Hrv.Hi again,
Thanks a lot Hrv.... :-)! I just finished re-converting the force based mesh motion solver I had written a while ago to use tet decomposition (I had used it in OF-1.3 with tet decomposition long time ago...), and am currently running a test case... Everything seems to be working perfectly fine, and I am looking forward to trying it on one of the more difficult cases tomorrow (hopefully!) So now its time to look through the paper from Zeljko... !! Shall indeed refer to the appropriate papers at every possible opportunity :-)! Philippose |

Hi everybody,
Sorry to answHi everybody,
Sorry to answer you after this kind support only now, but last week was really busy for me - but not only for work ;) I manage to download and use OpenFoam-1.4.1-dev (after some adventures were I try to compile it, but never succeed...I think I'm not really gifted for this kind of stuff)...and the binaries. So it's working now on my computer. I play a little with the solvers: **velocityLaplacian**(the same as in OpenFoam-1.4.1) give more or less the same results.**laplaceFaceDecomposition**seems to be more robust - for my case - but really slower. Maybe this is normal? (*"there is no free lunch"*)- To impose non-uniform condition, I'm really lost : I consider a face with 90 nodes and 44 faces. With
**velocityLaplacian**, in the file**pointMotionU**, I impose the 90 velocity at the 90 nodes...no problem ; with**laplaceFaceDecomposition**the solver asks for 134 values of velocities in the file**motionU**(I can imagine that is the nodal values + the face values...but in wich order? ). Is it possible to impose value only at nodes with**laplaceFaceDecomposition**? - I notice that I'm not able to use something like
**deformationEnergy**of**distorsionEnergy**with the solver**velocityLaplacian**. Is this normal? If or if not, do you have an example for the**dynamicMeshDict**file for this case? **displacement***solvers and especially**displacementSBRStress**ask for**pointDisplacement**files...this is logical. Do you think it is a good idea to use one of them - but for the testing problem i'm not really able to impose a displacement linearly depending of time for the moment - I will look maybe in this direction...
Thank you for answers, even If my questions are maybe not so clear ;) -- Christophe KASSIOTIS |

Heya:
- laplaceFaceDecomposHeya:
- laplaceFaceDecomposition is slow. Yes - cellDecomposition is faster. In order to get robustness I need more points and that is why. The best I can offer is cellDecomposition and then relax mesh motion convergence tolerances - in all cases, points go first, then face centres (face decomposition only) and then cell centres. - you've got mapping functions which will take point or cell data and interpolate to points or points/faces, depending on decomposition. Beware of compilation switches, it is very difficult to cleanly spearate this... - fancy diffusivities came from Zeljko's PhD and we did vertex-based motion. You should be able to move them to cell-based motion as well - the algorithm is the same, but field type and run-time selection tables are different. Enjoy, Hrv |

Thank you for the quick answerThank you for the quick answer Hrv,
When I want to use something like cellDecomposition, I get the following message: 7 ( displacementSBRStress pseudoSolidFaceDecomposition displacementComponentLaplacian velocityLaplacian displacementLaplacian laplaceFaceDecomposition velocityComponentLaplacian ) A small grep -r laplaceCellDecomposition give me as an answer the file tetDecompositionMotionSolver.H with the following lines seems to be of interest: #ifdef CELL_DECOMP TypeName("laplaceCellDecomposition"); #else TypeName("laplaceFaceDecomposition"); #endif If I understand what I read in the code and what you say: Quote:
src/tetDecompositionMotionSolver. Did I understand well ? If yes, how can I do this ? (I'm not the kind of guy who is able to compile thinks with flag in 1s http://www.cfd-online.com/OpenFOAM_D...part/happy.gif ). For instance, did I need to do a wmake . tetDecompositionMotionSolver with an option? I will also try to impose the good value for a laplaceFaceDecomposition solver with mapping fonction and say if I have some problems... Thank you CK |

You need to link cellDecomposiYou need to link cellDecompositionMotionSolver or recompile the application with CELL_DECOMP option.
Enjoy, Hrv |

Hello everybody,
Thank you Hello everybody,
Thank you again for answering Hrv; I have agains two questions: **laplaceFaceDecomposition**: seem to work really well when I impose at each face center a mean between the point velocity and allow really big deformations (see Picture**[2]**). However, for the moment, I'm doing this by "hand" in the input file. Do you think It can be possible to impose only value at point, and that OpenFOAM is doing the interpolation (i'm sure it is possible, but I don't know really were I have to modify things)**laplaceCellDecomposition**: I think I manage to make it work by "linking" (see code**[1]**). But I'm not sure it's really calling the good solver: the solver ask also for value at node center -- they are useless if I understood properly what is doing*cellDecomposition*as a decomposition...and more distrubing the results are exactly the same has*faceDecomposition*. Do you think I'm in fact calling an*faceDecomposition*solver ? Or the example I'm using don't give significant differences ( e.g. : motion too small, 2d ) ?
[1] : dynamicMeshDict file // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // dynamicFvMesh dynamicMotionSolverFvMesh; twoDMotion yes; motionSolverLibs ("libcellDecompositionMotionSolver.so"); solver laplaceCellDecomposition; diffusivity quadratic; frozenDiffusion off; distancePatches ( movingWall ); // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // [2] : moving Mesh pictures with a laplaceFaceDecomposition solver. Problem treated : imposed velocity for the "moving Wall" only in y direction, linearly depending of x (imposed at each node by "hand"). at time 0.46: <https://perso.crans.org/kassiotis/openfoam/mesh_laplacefacedecomposition_046_fac evelocitiymean.png> at time 0.46 with a zoom: <https://perso.crans.org/kassiotis/openfoam/mesh_laplacefacedecomposition_046_fac evelocitiymean_zoom.png> at time 1.00: <https://perso.crans.org/kassiotis/openfoam/mesh_laplacefacedecomposition_100_fac evelocitiymean.png> at time 1.00 with a zoom: <https://perso.crans.org/kassiotis/openfoam/mesh_laplacefacedecomposition_100_fac evelocitiymean_zoom.png> CK |

Sorry, cannot see the picturesSorry, cannot see the pictures.
Hrv |

Now it's working (due to a misNow it's working (due to a misspelling with majuscules).
CK |

Have a look at icoFsiFoam:
Have a look at icoFsiFoam:
pointVectorField solidPointsDispl = cpi.interpolate(Usolid - Usolid.oldTime()); vectorField fluidPatchPointsDispl = interpolatorSolidFluid.pointInterpolate ( solidPointsDispl.boundaryField()[solidPatchID]. patchInternalField() ); motionUFluidPatch == tppi.pointToPointInterpolate ( fluidPatchPointsDispl/runTime.deltaT().value() ); The first one takes the data on the solid patch (cell centres) and interpolates it into points. The second one takes the point data and interpolates from solid to fluid. The third one takes the point data (that is mesh points) and interpolates into whatever the motion solver wants: for cell decomposition it just uses cell data, for face decomposition it will do a face centre as well in a consistent manner. Have a look at tetPolyPatchInterpolation/tetPolyPatchInterpolationCellDecomp/tetPolyPatchInterp olationCellDecomp.H for other available functions, depending on whatther you know the motion on points or cell centres. //- Interpolate from faces to points template<class> tmp<field<type> > faceToPointInterpolate ( const Field<type>& ff ) const; template<class> tmp<field<type> > faceToPointInterpolate ( const tmp<field<type> >& tff ) const; //- Interpolate from mesh points to tet FEM points template<class> tmp<field<type> > pointToPointInterpolate ( const Field<type>& ff ) const; template<class> tmp<field<type> > pointToPointInterpolate ( const tmp<field<type> >& tff ) const; Enjoy, Hrv |

For the one interested, I haveFor the one interested, I have made a short rapport on the moving mesh subject. Hope that will help someone.
Please, be kind with my (poor) English ! And remind this is only a draft for the moment http://www.cfd-online.com/OpenFOAM_D...part/happy.gif <https://perso.crans.org/kassiotis/op...movingmesh.pdf> CK |

Hello,
Hrv, I noticed your Hello,
Hrv, I noticed your first post in this thread mentioned simulations of airfoils with sharp trailing edges.. I have been working on some NACA0012 simulations and seem to be having trouble with the potential solution at the trailing edge. (Note laminar and turbulent simulations are working fine) The problem is that at an angle of attack, the velocity field tries to "bend" around the sharp trailing edge i.e. the first mesh points surrounding the TE point go from very high velocity on the pressure side through to low velocity on the suction side of the wing. The cell point on the tip of the sharp TE is approximately the average of the values surrounding it. Case set-up is: 2D rectangular domain, rotated about the airfoil for an angle of attack tetrahedral mesh (thanks gmsh) airfoil: slip boundary (have also tried symmetryPlane) inlet, top, bottom: U = 10m/s, p = zeroGradient outlet: U = zeroGradient, p = 0 Schemes are all from the tutorial, except I'm using 6 orthogonal correctors because of the tetrahedral mesh. I have tried chopping off the sharp edge, and increasing the mesh density around the blunt edge but the same problem persists near the square edges. Also it is not really a suitable solution for me because unfortunately the shape of the TE matters for what I am trying to do. Do you (or anyone else!) know how to solve this? Thank you, Richard. |

Essentially, how do I apply thEssentially, how do I apply the Kutta-Joukowski condition on the TE?
R |

well, if what you are after iswell, if what you are after is only the potential-flow solution around a lifting body, you are better off using a panel method (simpler and cheaper).
If you really want to stick to the FVM for that (a bit of an overkill), try and enforce a zero velocity on the 2 airfoil cell faces sharing the trailing edge (define them as a separate patch). That could do the trick for 2D airfoils with non-cusped TE. Patrick |

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