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October 1, 2018, 09:48 |
Sudden contration
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#1 |
Member
Anders Dyhr Nørløv
Join Date: Aug 2018
Posts: 32
Rep Power: 8 |
Hello
I'm trying to learn to use OpenFOAM. For that purpose I tried to simulate a sudden contration of a circular pipe. I go from 80 mm to 40 mm see image below (clipped trough the half), where the inlet is the 80 mm. geometry.PNG When i run it runs fine, but when i check the results in paraview I get a pressure drop of 50. Converting it to bar using the density of water of 998, I get a pressure drop of 0.5 bar. When I try to calculate the pressure drop in a manual way (fx. using http://www.pressure-drop.mobi/0303.html) i get a pressure drop of 0.13 bar. Changing the inlet velocity I always get roughly a factor of 4 between the two methods. I suspect that I'm doing something completely wrong in my simulation, but I don't know what it is. I know one of the difficult things with CFD is to choose sensible parameters, so maybe that is where i'm going wrong. Any help is much appreciated. Iøve created teh mesh with salome and used ideasUnvToFoam to create the mesh in OpenFOAM, you can see my mesh here (I know it is a bit coarse, but I thought it would still give a sensible result): mesh.PNG I've tried to setup the simpleFoam solver with the following parameters: Code:
/*--------------------------------*- C++ -*----------------------------------*\ | ========= | | | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox | | \\ / O peration | Version: v1806 | | \\ / A nd | Web: www.OpenFOAM.com | | \\/ M anipulation | | \*---------------------------------------------------------------------------*/ FoamFile { version 2.0; format ascii; class volVectorField; object U; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // dimensions [0 1 -1 0 0 0 0]; internalField uniform (0 0 0); boundaryField { channel_closed_solid_inlet { type fixedValue; value uniform (0 2 0); } channel_closed_solid_outlet { type zeroGradient; } channel_closed_solid_walls { type fixedValue; value uniform (0 0 0); } } // ************************************************************************* // Code:
/*--------------------------------*- C++ -*----------------------------------*\ | ========= | | | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox | | \\ / O peration | Version: v1806 | | \\ / A nd | Web: www.OpenFOAM.com | | \\/ M anipulation | | \*---------------------------------------------------------------------------*/ FoamFile { version 2.0; format ascii; class volScalarField; object p; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // dimensions [0 2 -2 0 0 0 0]; internalField uniform 0; boundaryField { channel_closed_solid_inlet { type zeroGradient; } channel_closed_solid_outlet { type fixedValue; value uniform 0; } channel_closed_solid_walls { type zeroGradient; } } // ************************************************************************* // Code:
/*--------------------------------*- C++ -*----------------------------------*\ | ========= | | | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox | | \\ / O peration | Version: v1806 | | \\ / A nd | Web: www.OpenFOAM.com | | \\/ M anipulation | | \*---------------------------------------------------------------------------*/ FoamFile { version 2.0; format ascii; class volScalarField; location "0"; object k; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // dimensions [0 2 -2 0 0 0 0]; internalField uniform 0.024576; boundaryField { channel_closed_solid_inlet { type fixedValue; value uniform 0.024576; } channel_closed_solid_outlet { type zeroGradient; } channel_closed_solid_walls { type kqRWallFunction; value uniform 0.024576; } } // ************************************************************************* // Code:
/*--------------------------------*- C++ -*----------------------------------*\ | ========= | | | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox | | \\ / O peration | Version: v1806 | | \\ / A nd | Web: www.OpenFOAM.com | | \\/ M anipulation | | \*---------------------------------------------------------------------------*/ FoamFile { version 2.0; format ascii; class volScalarField; location "0"; object epsilon; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // dimensions [0 2 -3 0 0 0 0]; internalField uniform 0.113; boundaryField { channel_closed_solid_inlet { type fixedValue; value uniform 0.113; } channel_closed_solid_outlet { type zeroGradient; } channel_closed_solid_walls { type epsilonWallFunction; value uniform 0.113; } } // ************************************************************************* // Code:
/*--------------------------------*- C++ -*----------------------------------*\ | ========= | | | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox | | \\ / O peration | Version: v1806 | | \\ / A nd | Web: www.OpenFOAM.com | | \\/ M anipulation | | \*---------------------------------------------------------------------------*/ FoamFile { version 2.0; format ascii; class volScalarField; location "0"; object nut; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // dimensions [0 2 -1 0 0 0 0]; internalField uniform 0; boundaryField { channel_closed_solid_inlet { type calculated; value uniform 0; } channel_closed_solid_outlet { type calculated; value uniform 0; } channel_closed_solid_walls { type nutkWallFunction; value uniform 0; } } // ************************************************************************* // Code:
/*--------------------------------*- C++ -*----------------------------------*\ | ========= | | | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox | | \\ / O peration | Version: v1806 | | \\ / A nd | Web: www.OpenFOAM.com | | \\/ M anipulation | | \*---------------------------------------------------------------------------*/ FoamFile { version 2.0; format ascii; class dictionary; location "constant"; object turbulenceProperties; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // simulationType RAS; RAS { // Tested with kEpsilon, realizableKE, kOmega, kOmegaSST, v2f, // ShihQuadraticKE, LienCubicKE. RASModel kEpsilon; turbulence on; printCoeffs on; } // ************************************************************************* // Code:
/*--------------------------------*- C++ -*----------------------------------*\ | ========= | | | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox | | \\ / O peration | Version: v1806 | | \\ / A nd | Web: www.OpenFOAM.com | | \\/ M anipulation | | \*---------------------------------------------------------------------------*/ FoamFile { version 2.0; format ascii; class dictionary; location "constant"; object transportProperties; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // transportModel Newtonian; nu nu [0 2 -1 0 0 0 0] 1e-6; CrossPowerLawCoeffs { nu0 nu0 [0 2 -1 0 0 0 0] 1e-6; nuInf nuInf [0 2 -1 0 0 0 0 ] 1e-6; m m [0 0 1 0 0 0 0] 1; n n [0 0 0 0 0 0 0] 1; } BirdCarreuCoeffs { nu0 nu0 [0 2 -1 0 0 0 0] 1e-6; nuInf nuInf [0 2 -1 0 0 0 0 ] 1e-6; k k [0 0 1 0 0 0 0] 0; n n [0 0 0 0 0 0 0] 1; } // ************************************************************************* // Code:
/*--------------------------------*- C++ -*----------------------------------*\ | ========= | | | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox | | \\ / O peration | Version: v1806 | | \\ / A nd | Web: www.OpenFOAM.com | | \\/ M anipulation | | \*---------------------------------------------------------------------------*/ FoamFile { version 2.0; format ascii; class dictionary; location "system"; object controlDict; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // application simpleFoam; startFrom latestTime; startTime 0; stopAt endTime; endTime 2000; deltaT 1; writeControl timeStep; writeInterval 100; purgeWrite 0; writeFormat ascii; writePrecision 6; writeCompression off; timeFormat general; timePrecision 6; runTimeModifiable true; // ************************************************************************* // Code:
/*--------------------------------*- C++ -*----------------------------------*\ | ========= | | | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox | | \\ / O peration | Version: v1806 | | \\ / A nd | Web: www.OpenFOAM.com | | \\/ M anipulation | | \*---------------------------------------------------------------------------*/ FoamFile { version 2.0; format ascii; class dictionary; location "system"; object fvSchemes; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // ddtSchemes { default steadyState; } gradSchemes { default Gauss linear; } divSchemes { default none; div(phi,U) Gauss upwind; div(phi,k) Gauss upwind; div(phi,epsilon) Gauss upwind; div(phi,R) Gauss upwind; div(R) Gauss linear; div(phi,nuTilda) Gauss upwind; div((nuEff*dev2(T(grad(U))))) Gauss linear; } laplacianSchemes { default Gauss linear corrected; } interpolationSchemes { default linear; } snGradSchemes { default corrected; } wallDist { method meshWave; } // ************************************************************************* // Code:
/*--------------------------------*- C++ -*----------------------------------*\ | ========= | | | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox | | \\ / O peration | Version: v1806 | | \\ / A nd | Web: www.OpenFOAM.com | | \\/ M anipulation | | \*---------------------------------------------------------------------------*/ FoamFile { version 2.0; format ascii; class dictionary; location "system"; object fvSolution; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // solvers { p { solver GAMG; tolerance 1e-06; relTol 1e-06; smoother GaussSeidel; nPreSweeps 0; nPostSweeps 2; cacheAgglomeration on; nCellsInCoarsestLevel 10; mergeLevelse 1; } "(U|k|epsilon|R|nuTilda)" { solver smoothSolver; smoother symGaussSeidel; tolerance 1e-06; relTol 1e-06; } } SIMPLE { nNonOrthogonalCorrectors 0; } relaxationFactors { fields { p 0.3; } equations { U 0.3; k 0.3; epsilon 0.3; R 0.3; nuTilda 0.3; } } // ************************************************************************* // |
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October 2, 2018, 05:03 |
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#2 |
Senior Member
Gerhard Holzinger
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Location: Austria
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Check whether your y+ values at the walls are in the appropriate range. Being off can cause a faulty prediction of the pressure loss. Alternatively, you could try running the case using the kOmega model.
Furthermore, the mesh is not all that beautiful. |
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October 2, 2018, 05:23 |
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#3 |
Member
Anders Dyhr Nørløv
Join Date: Aug 2018
Posts: 32
Rep Power: 8 |
Thanks for the suggestions. I checked the yPlus values (didn't know about them, thanks for that), and they are way to high. Also I agree that the mesh is not good.
I use salome to mesh, and I'm also new using that. I tried to make the mesh better. What do you think about this new mesh? Looks better? mesh_fine.jpg |
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October 2, 2018, 07:20 |
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#4 |
Senior Member
Uwe Pilz
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If a model allows manual meshing you should go that way. In you case it is straightforward.
If you look closely at the meshes the have strange regions both. But I don't believe that your problem depends on that. ~ Which Re number did you use? May be there is a problem with the turbulence calculation. Pressure drops differ widely between laminar and turbulent flow.
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Uwe Pilz -- Die der Hauptbewegung überlagerte Schwankungsbewegung ist in ihren Einzelheiten so hoffnungslos kompliziert, daß ihre theoretische Berechnung aussichtslos erscheint. (Hermann Schlichting, 1950) |
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October 2, 2018, 07:27 |
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#5 |
Member
Anders Dyhr Nørløv
Join Date: Aug 2018
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The Reynolds number is very high. I think in the region of 200000 - 300000. You don't mean that it should be set somewhere in OpenFOAM do you? Or do you mean when I calculated the k and epsilon values?
Not sure what you mean by manual mesh? How do I do that? |
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October 2, 2018, 08:11 |
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#6 |
Member
Anders Dyhr Nørløv
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Should I actually calculate different k and epsilon for the pipe walls with the large diameter and the small diameter?
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October 2, 2018, 13:09 |
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#7 |
Senior Member
Uwe Pilz
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> Reynolds number is very high...200000 - 300000
I recommend starting with lower Re numbers and looking what happens. > what you mean by manual mesh? How do I do that? blockMesh.
__________________
Uwe Pilz -- Die der Hauptbewegung überlagerte Schwankungsbewegung ist in ihren Einzelheiten so hoffnungslos kompliziert, daß ihre theoretische Berechnung aussichtslos erscheint. (Hermann Schlichting, 1950) |
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October 3, 2018, 04:13 |
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#8 |
Member
Anders Dyhr Nørløv
Join Date: Aug 2018
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The reason I used Salome to do the mesh, was because I'm investigation how a OpenFOAM workflow can be implemented at our company, and in general the geometries will be very complex.
I tried going down to a speed of 0.1 m/s, and a Re below 20000. I still get a factor of 4 between the manual calculation and OpenFOAM. I think my convergence and yPlus is OK? Code:
smoothSolver: Solving for Ux, Initial residual = 1.22094e-07, Final residual = 1.22094e-07, No Iterations 0 smoothSolver: Solving for Uy, Initial residual = 1.6853e-08, Final residual = 1.6853e-08, No Iterations 0 smoothSolver: Solving for Uz, Initial residual = 1.25779e-07, Final residual = 1.25779e-07, No Iterations 0 GAMG: Solving for p, Initial residual = 8.73275e-07, Final residual = 8.73275e-07, No Iterations 0 GAMG: Solving for p, Initial residual = 8.73275e-07, Final residual = 8.73275e-07, No Iterations 0 time step continuity errors : sum local = 2.53288e-06, global = 5.52101e-08, cumulative = -6.2634e-06 smoothSolver: Solving for epsilon, Initial residual = 7.9535e-07, Final residual = 7.9535e-07, No Iterations 0 smoothSolver: Solving for k, Initial residual = 9.04923e-07, Final residual = 9.04923e-07, No Iterations 0 ExecutionTime = 264.54 s ClockTime = 265 s Code:
patch channel_closed_solid_walls_large y+ : min = 0.482836, max = 14.916, average = 4.53306 patch channel_closed_solid_walls_small y+ : min = 6.79218, max = 48.9457, average = 23.8934 |
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October 3, 2018, 06:38 |
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#9 |
Senior Member
Uwe Pilz
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> ecause I'm investigation how a OpenFOAM workflow can be implemented at our company
I don't think that it works that way. OF (and other cfd software) is not some kind of advanced pocket computer. You need experience how to work with it. This includes a strategy to ensure the correctness of your results.
__________________
Uwe Pilz -- Die der Hauptbewegung überlagerte Schwankungsbewegung ist in ihren Einzelheiten so hoffnungslos kompliziert, daß ihre theoretische Berechnung aussichtslos erscheint. (Hermann Schlichting, 1950) |
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October 3, 2018, 07:01 |
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#10 |
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Anders Dyhr Nørløv
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Yeah, I agree. This is a preliminary study to see how one can work with OpenFOAM. I think it is possible to study the workflow. That is how will we take a given component from design, to mesh, to solving, and if this is a viable way of working (or we need to invest in expensive commercial programs). I think my conclusion is that it is definetely possible to use OpenFOAM, and I like the fact that it is open source and c++, because as a physicists and c++ programmer, I see the possibility to program special cases important for our company in the future.
If we see that that is possible, and we find that it is worth investing money and time in it, we will start getting help from the outside, in form of courses and support, to gain more experience in these kind of simulations. I'm fully aware that it is not hard to get OpenFOAM up and running, but it is very difficult to make correct assumptions and interpretations of the results. Something we have to invest a lot of time in to be able to do. My question here was more if someone could see why I didn't get my results to match, my simple calculations made by empiric formulas (formulas we have seen match experiments very well). If it is not possible to do so, and we need more training and experience to do it correctly, we will take that into considerations. Justed hoped that someone maybe had experience with simulating a contraction, and knew how to simulate it, or knew if precise results could be expected. It could be that with CFD you can not expect to get results more precise than within a factor of 5, and that my simulation was succesfull (hope not ). If that is the case that is also fine, but then we need to take that into considerations. |
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October 3, 2018, 08:41 |
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#11 |
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Michael Alletto
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Hello,
did you try the have prism layers close to the wall? Usually tetrahedra are too diffusive to accurately solve the wall shear stress close to the wall. Besides this they introduce an additional diffusion due to the fact that the flow is not normal to the cell face. So I strongly advise to use a high quality mesh close to the wall to accurately resolve the transport phenomena which are leading to the two recirculation regions in front upwind and downwind of the contraction. In addition it is best practice (if the computational costs allows it) to have a y+ ~ 1 at the wall in order to avoid the usage of wall function which are known to not correctly reproduce separated flows. Best Michael |
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October 3, 2018, 09:35 |
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#12 |
Member
Anders Dyhr Nørløv
Join Date: Aug 2018
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Hello
If I don't use wallfunctions what should i use for type in the k and epsilon files? |
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October 3, 2018, 09:56 |
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#13 |
Senior Member
Uwe Pilz
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> It could be that with CFD you can not expect to get results more precise than within a factor of 5
You may expect much better results. Start with a simple geometry, a simple physics (low to medium Re) and an straightforward mesh. Look what happens and change one variable after the other. You try - without experience - using a mesh of doubtful quality - consisting of tetraeder elements (instead of heaxaeder) - to calculate an example withe high Reynolds number. Too much complications for the start.
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Uwe Pilz -- Die der Hauptbewegung überlagerte Schwankungsbewegung ist in ihren Einzelheiten so hoffnungslos kompliziert, daß ihre theoretische Berechnung aussichtslos erscheint. (Hermann Schlichting, 1950) |
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October 3, 2018, 17:12 |
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#14 | |
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Geir Karlsen
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Quote:
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October 4, 2018, 03:02 |
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#15 |
Member
Anders Dyhr Nørløv
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Thanks for the great link. I was actually looking into using hex mesh. I guess the work flow will then be to prepare stl files in salome, and then use snappyHexMesh to create the mesh.
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October 4, 2018, 03:12 |
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#16 | |
Super Moderator
Tobias Holzmann
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Hi Karlsen,
thank you very much for mentioning my screencast in that way. I feel honored. An additional information to the screencasts: Quote:
Good luck & as Karlsen mentioned, hex-dominant meshes are much better in a numerical sense. E.g., second order linear scheme and tet meshes for pure convection: https://www.youtube.com/watch?v=C0CcN7l37Fg Additionally, as Gerhard said, the turbulence model can influence your solution (I am not a turbulence guy; therefore I cannot give you any feedback). A few hints for open source software in general (if one is interested - valid for everybody) - the above content is not related to the topic ================================================== ======================================= Furthermore, I want to make one statement to OpenFOAM and Open Source software that many people do not or don´t want to recognize. I published my material for more than five years for free till mid of 2018. Therefore I know the following circumstances:
In other words, doing a CFD analysis with 19 cells will not make sense at all. However, if you have 76.000 cells, you can do pretty cool things, don´t you? Okay, some people think they need 600.000.000 cells for their problems It sounds a bit of advertising to donate to OpenFOAM, to my work or other open source software but it is not. I want to make you sensitive, that it is not naturally that open source software is free forever. My wish for the future would be: If people are using open source software, they should give something back regarding:
An excellent example that people thought a natural free material is forever free is my material - it´s closed now (most of the stuff); You don´t believe how many emails I got, questioning when it is available again ================================================== ======================================= Enough of my talk. I hope that the hints at the beginning help to resolve the problem. Another option is that you post your case that we can check out the stuff in more detail. Additionally, the equation and reference to the equation would be beautiful to have; I expect that you use simple Bernoulli equation? Further information for OpenFOAM
new things are added from time to time.
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Keep foaming, Tobias Holzmann Last edited by Tobi; October 4, 2018 at 06:38. |
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October 4, 2018, 03:32 |
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#17 |
Member
Anders Dyhr Nørløv
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Thank you so much for taking your time to help me with such a detailed answer.
Just a couple of questions: The boundary layer has to establish first, using a fixedValue will not give you a boundary layer. Thus, this layer has to be established first (I am not sure if this will influence the results drastically). However, it is worth to know that your inlet boundary condition can influence the phenomenon you are interested in; a rule of thumb is, e.g., for the pipe diameter of 100 mm, the pipe inlet - before the contraction - should be at least 300 mm away. Related to the hint mentioned above, a parabolic inlet profile would be recommended. I will try to extend the length of the pipe before and after the contraction to give time to make the flow develop. Not sure about the fixedValue thing, should I change the boundary condition, or will the extended pipe length with the fixedValue boundary condition, develop a boundary layer? Change the inlet values for k and epsilon to turbulentKinetic... and mixingLength.... I will try this. During my master study, we made such tests too. However, after the contraction, we had the expansion immediately and recorded the pressure drop before and behind the contraction. The comparison to the analytical solution was 99.99%. Therefore, I expect that there is something wrong in your set-up. Great news Furthermore, you should be aware of your first order scheme. Not sure what you mean by this? Summing up, there are still plenty of things you can consider improving your simulation. However, a discrepancy of 2.5 bar is a bit too high. What comes into my mind, please be aware of the pressure you set. It is not the real pressure. The differences \delta p are fine but absolute values are different. As far as I understand it is the pressure divided by density? Or do you mean that the pressures are not the absolute pressure, because I set my reference at the outlet to zero? |
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October 4, 2018, 04:29 |
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#18 | |
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Michael Alletto
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Wall function usage |
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October 4, 2018, 06:38 |
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#19 | |
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Tobias Holzmann
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Quote:
Quote:
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Keep foaming, Tobias Holzmann |
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October 9, 2018, 06:29 |
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#20 |
Member
Anders Dyhr Nørløv
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Thanks for all the suggestions.
I've tried to use the suggestions. First of all I've tried learning some snappyHexMesh to genererate a better hexagonal mesh, and elongated the pipe length. I now have the following mesh: grid.PNG gridzoom1.PNG gridzoom2.PNG As you can see the grid is much finer especially at the walls. However, there are still some strange cell's, don't know if that is a problem. The finer mesh is generating more of the expected turbulence in the corners and just after the contraction. However, i still get a too high pressure drop over the contraction compared to the empirical formula. result.PNG As you can see the pressure drop is between 3.8 to 3.2 coresponding to 32 mbar and 38 mbar for water. The empirical formula suggest 8 mbar for a flow of 0.5 m/s. I've also tried using the suggestied boundary conditions Code:
/*--------------------------------*- C++ -*----------------------------------*\ | ========= | | | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox | | \\ / O peration | Version: v1806 | | \\ / A nd | Web: www.OpenFOAM.com | | \\/ M anipulation | | \*---------------------------------------------------------------------------*/ FoamFile { version 2.0; format ascii; class volScalarField; location "0"; object epsilon; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // dimensions [0 2 -3 0 0 0 0]; internalField uniform 0.00031185580835531597; boundaryField { inlet { type turbulentMixingLengthDissipationRateInlet; mixingLength 0.05; value 1; } outlet { type zeroGradient; } wall_large { //type zeroGradient; type epsilonWallFunction; value uniform 0.0000031185580835531597; } wall_small { //type zeroGradient; type epsilonWallFunction; value uniform 0.000008088538952456775; } } // ************************************************************************* // Code:
/*--------------------------------*- C++ -*----------------------------------*\ | ========= | | | \\ / F ield | OpenFOAM: The Open Source CFD Toolbox | | \\ / O peration | Version: v1806 | | \\ / A nd | Web: www.OpenFOAM.com | | \\/ M anipulation | | \*---------------------------------------------------------------------------*/ FoamFile { version 2.0; format ascii; class volScalarField; location "0"; object k; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // dimensions [0 2 -2 0 0 0 0]; internalField uniform 0.000040603056516117657; boundaryField { inlet { type turbulentIntensityKineticEnergyInlet; intensity 0.05; value 1; } outlet { type zeroGradient; } wall_large { //type zeroGradient; type kqRWallFunction; value uniform 0.000040603056516117657; } wall_small { //type zeroGradient; type kqRWallFunction; value uniform 0.00004828544369982472; } } // ************************************************************************* // So all in all I like the new grid, and the ability to see turbulence effects with flow lines, but the pressure drop is still just as much off. More suggestions how to improve my simulation? |
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