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February 11, 2013, 10:53 |
Convergence problem
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#1 |
Member
xxxxx
Join Date: Feb 2013
Posts: 34
Rep Power: 13 |
Hello everybody,
I'm trying to run a case with simpleFoam. It's a stationary simulation with k-espilon turbulence model. Initially it seems the simulation is converging but after some step suddenly the residuals show a strange behaviour and from this on the results have no phisical sense. I attach the residuals vs iteration plot. Is there anyone who can help me? I tryied to make modification to the mesh, to the relaxation factor and to the fvScheme but I wasn't able to solve the problem. |
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February 11, 2013, 12:52 |
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#2 |
Senior Member
Ehsan
Join Date: Oct 2012
Location: Iran
Posts: 2,208
Rep Power: 27 |
i have a problem like you.whats your case?do you have some region of high gradients?
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February 11, 2013, 13:54 |
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#3 |
Senior Member
Daniele Vicario
Join Date: Mar 2009
Location: Novara, Italy
Posts: 142
Rep Power: 17 |
Can you send your controlDict / fvSolution and fvScheme ?
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Daniele Vicario blueCFD2.1 - Windows 7 |
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February 11, 2013, 15:47 |
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#4 |
Senior Member
Ehsan
Join Date: Oct 2012
Location: Iran
Posts: 2,208
Rep Power: 27 |
I use compressible solvers like rhoPimpleFoam but now changing to sonicFoam.
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February 11, 2013, 16:00 |
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#5 |
Senior Member
Ehsan
Join Date: Oct 2012
Location: Iran
Posts: 2,208
Rep Power: 27 |
Code:
application rhoPimpleFoam; startFrom latestTime; startTime 0; stopAt endTime; endTime .02;//0.020708089 deltaT 5.6e-9; writeControl adjustableRunTime; writeInterval .000001; purgeWrite 0; writeFormat binary; writePrecision 10; writeCompression on; timeFormat general; timePrecision 6; runTimeModifiable true; adjustTimeStep yes; maxCo 0.1; maxDeltaT .0001; libs ( "libOpenFOAM.so" "libgroovyBC.so" ) ; Code:
ddtSchemes { default backward; } gradSchemes { default Gauss linear; grad(p) Gauss linear; grad(U) Gauss linear;//cellLimited leastSquares 1.0 } divSchemes { default none; div(phi,U) Gauss upwind; div(phid,p) Gauss upwind;// upwind div(phi,K) Gauss upwind; div(phi,h) Gauss upwind; div(phi,k) Gauss upwind; div(phi,epsilon) Gauss upwind; div(phi,R) Gauss upwind; div(phi,omega) Gauss upwind; div((rho*R)) Gauss limitedLinear 1; div(R) Gauss limitedLinear 1; div(U) Gauss limitedLinear 1; div((muEff*dev2(T(grad(U))))) Gauss linear; div(tauMC) Gauss linear; } laplacianSchemes { default Gauss linear limited .5;//limited .5 /*laplacian(muEff,U) Gauss linear corrected; laplacian(mut,U) Gauss linear corrected; laplacian(DkEff,k) Gauss linear corrected; laplacian(DepsilonEff,epsilon) Gauss linear corrected; laplacian(DREff,R) Gauss linear corrected; laplacian(DomegaEff,omega) Gauss linear corrected; laplacian((rho*(1|A(U))),p) Gauss linear corrected; laplacian(alphaEff,h) Gauss linear corrected; laplacian(k,T) Gauss linear corrected; laplacian(alpha,e) Gauss linear corrected; laplacian(alphaEff,e) Gauss linear corrected;*/ } interpolationSchemes { default linear; } snGradSchemes { default limited .5;//corrected } fluxRequired { default no; p ; } Code:
solvers { p { solver PCG; preconditioner DIC; tolerance 1e-13; relTol 0; maxIter 25000; /*solver GAMG; smoother DICGaussSeidel; cacheAgglomeration true; nCellsInCoarsestLevel 200; nPreSweeps 0; nPostSweeps 2; nFinestSweeps 2; agglomerator faceAreaPair; mergeLevels 2; tolerance 1e-012; relTol 0;*/ } pFinal { $p; relTol 0; } "rho.*" { $p; tolerance 1e-11; relTol 0; } "(U|e|h|R|k|epsilon|omega)" { solver PBiCG; preconditioner DILU; tolerance 1e-11; relTol 0; maxIter 25000; } "(U|h|R|k|epsilon|omega)Final" { $U; relTol 0; } } PIMPLE { momentumPredictor yes; nOuterCorrectors 4; nCorrectors 3; nNonOrthogonalCorrectors 0; rhoMin rhoMin [ 1 -3 0 0 0 ] 0.5; rhoMax rhoMax [ 1 -3 0 0 0 ] 6; residualControl { "(U|k|omega)" { relTol 0; tolerance 0.00000000001; } } } |
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February 11, 2013, 17:22 |
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#6 |
Member
xxxxx
Join Date: Feb 2013
Posts: 34
Rep Power: 13 |
Thanks for your answers.
My case is steasy state incompressible flow in a duct of quite complex geometry. I tried to simplify the geometry by removing chamfers and small details. The mesh is unstructured, with boundary layer, about 500'000 nodes. I noticed that, since some iterations before the computation failed, the mass flow continuity started not to be satisfied. Then in some region of the mesh the values of velocity or pressure rise suddenly. When I change the mesh and restart another simulation the point in which the anomalous values appears mooves. When i do the checkMesh i don't find any error or warning. The skew value is around 0.7 . I tried to change the fvScheme. I set 1st order scheme everywere. This allowed me to make the simulation run for 1 hundred iteration more before to have the same problem. Does anyone have an idea of the causes? |
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February 13, 2013, 16:36 |
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#7 |
Member
xxxxx
Join Date: Feb 2013
Posts: 34
Rep Power: 13 |
Please, can someone answer to some dubts?
1- when computing a simulation, should one let it run without modify relaxation factors or is it possible/advised to modify them? It happens that changing a relaxation factor completely changes the convergence. But is it right to do so? 2- how can i understand when the simulation is converged? Sometimes it happens that although the residuals are low, the results have no physical sense. On the other hand, sometimes although the residuals are high macroscopic quantities ,pressure drop for example, do not change much through time steps and results seem to be quite good. Is there any way to be quite sure that simulation has reached convergence? |
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February 15, 2013, 07:16 |
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#8 |
Senior Member
Daniele Vicario
Join Date: Mar 2009
Location: Novara, Italy
Posts: 142
Rep Power: 17 |
Without posting the necessary info (http://www.cfd-online.com/Forums/ope...tml#post351052) it's difficult to help you.
I had a similar problem regarding mass flow rate in a tet mesh... just a blind hint: in your fvsolution use relTol=0 for p.
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Daniele Vicario blueCFD2.1 - Windows 7 |
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