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June 3, 2013, 08:11 
forced convection of air inside a heated rectangular channel

#1 
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ankur
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Hey,
I am simulating the forced convection of air inside a heated rectangular channel. The air velocity is 1 m/s at the inlet. The temperature of the all four walls is 400 K and air is at 300 K. Initially I have taken the case of pitzdaily in simpleFoam solver and included the energy equation to incorporate the heat transfer. Then I used buoyantBoussinesqPimpleFoam solver but I am not able to get the convergence in pressure. I have given the velocity in x direction, but it does not show any velocity in that direction, instead it is showing the effect of buoyancy only, and show the circulating cells. I have tried the totalPressure, fixedPressure boundary conditions at the inlet and zeroGradient at the outlet, but no improvement. I am using kEpsilon model with first order upwind. For testing purpose the grid is a bit coarser. I am able to run the case without energy equation successfully with the simpleFoam solver, but problem comes whenever I include the energy equation. Please help me, it seems an easy problem but I am really stuck... Thanks Ankur 

June 4, 2013, 03:23 

#2 
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ankur
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Hey
I just checked my results. The velocity vectors are showing that the velocity reaches to zero value near the outlet. It is non physical as velocity should be 1 m/s everywhere. I am attaching the snapshot. I dont know what is happening. Please have a look. 

June 5, 2013, 06:38 

#4 
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ankur
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Hey
I found the solution to my earlier problem, Now the problem is different and the velocity which is 1 m/s at the inlet is going above to 1.14 m/s at the outlet. I am posting the case files and snapshot. I have made a silly mistake in the calculation of epsilon. I will get back to you once fix it. To get the pure forced convection my gravity and expansion coefficients are both zero. 

June 5, 2013, 06:50 

#5 
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ankur
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The problem remains same with correct calculations also. I am attaching more files now. The velocity is going beyond its correct value.


June 5, 2013, 07:19 

#6 
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Perhaps you should try buoyantPressure BC for the pressure at the inlet and outlet. This is the "perturbation" pressure that you are referring to, correct?


June 5, 2013, 07:42 

#7 
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ankur
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Hey Deji
I do not understand your reply. I have taken zero gravity so do you still think It will work? secondly I tried it but it is diverging. Now pressure is also converging but the velocity is going beyond its value as I posted above. Thanks 

June 5, 2013, 08:10 

#8  
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Tushar Chourushi
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Quote:
What do you mean to say by the mentioned Quote? Are you running your own solver "simpleFoam" with included energy equation in to it? 

June 5, 2013, 08:13 

#9 
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ankur
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Hey Tushar
Good to see your reply again.. No I am using my own solver. Sorry for the language. It meant when I shifted from simpleFoam to buoyantBoussinesqSimpleFoam. It seems to be a bit easy problem but I am getting strange velocity increment at the outlet. And the case I have taken is with very coarse grids, dimensions 0.1 X 0.05 X 0.5 with 17000 hexa cells. 

June 5, 2013, 08:16 

#10 
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My mistake. Since g is set to zero, that BC would be invalid.


June 5, 2013, 08:19 

#11 
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It seems like your flow is accelerating inside the channel due to a negative pressure gradient, dP/dx. What kind of pressure boundaries do you have at the inlet and outlet? And is this pressure the "perturbation pressure"?


June 5, 2013, 08:22 

#12 
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ankur
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Hey Deji
Thanks for the reply.. I am using zeroGradient at the inlet and fixedvalue (uniform 0) at the outlet. I am sorry but I dont know the meaning of perturbation pressure. Normally the simulation runs fine with these BCs when heating is not there. 

June 5, 2013, 08:26 

#13 
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Do me a favor, look in solver and paste the pressure equation and how the pressure is solved. You are probably solving a pressure equation, I would think.


June 5, 2013, 08:33 

#14 
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ankur
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Hey
I think I got the perturbation pressure, is it the pressure correction term in the SIMPLE algorithm? Here is the solver 00002 volScalarField rUA("rUA", 1.0/UEqn().A()); 00003 surfaceScalarField rUAf("(1A(U))", fvc::interpolate(rUA)); 00004 00005 U = rUA*UEqn().H(); 00006 UEqn.clear(); 00007 00008 phi = fvc::interpolate(U) & mesh.Sf(); 00009 adjustPhi(phi, U, p_rgh); 00010 00011 surfaceScalarField buoyancyPhi = rUAf*ghf*fvc::snGrad(rhok)*mesh.magSf(); 00012 phi = buoyancyPhi; 00013 00014 for (int nonOrth=0; nonOrth<=nNonOrthCorr; nonOrth++) 00015 { 00016 fvScalarMatrix p_rghEqn 00017 ( 00018 fvm::laplacian(rUAf, p_rgh) == fvc::div(phi) 00019 ); 00020 00021 p_rghEqn.setReference(pRefCell, getRefCellValue(p_rgh, pRefCell)); 00022 00023 // retain the residual from the first iteration 00024 if (nonOrth == 0) 00025 { 00026 eqnResidual = p_rghEqn.solve().initialResidual(); 00027 maxResidual = max(eqnResidual, maxResidual); 00028 } 00029 else 00030 { 00031 p_rghEqn.solve(); 00032 } 00033 00034 if (nonOrth == nNonOrthCorr) 00035 { 00036 // Calculate the conservative fluxes 00037 phi = p_rghEqn.flux(); 00038 00039 // Explicitly relax pressure for momentum corrector 00040 p_rgh.relax(); 00041 00042 // Correct the momentum source with the pressure gradient flux 00043 // calculated from the relaxed pressure 00044 U = rUA*fvc::reconstruct((buoyancyPhi + p_rghEqn.flux())/rUAf); 00045 U.correctBoundaryConditions(); 00046 } 00047 } 00048 00049 #include <finiteVolume/continuityErrs.H> 00050 00051 p = p_rgh + rhok*gh; 00052 00053 if (p_rgh.needReference()) 00054 { 00055 p += dimensionedScalar 00056 ( 00057 "p", 00058 p.dimensions(), 00059 pRefValue  getRefCellValue(p, pRefCell) 00060 ); 00061 p_rgh = p  rhok*gh; 00062 } 00063 } 

June 6, 2013, 00:02 

#15 
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Tushar Chourushi
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Hello Ank,
Since, Boussinesq approximation is used for the pressure, as you are using buoyantBoussinesqSimpleFoam. So, you need to provide the BC for p_rgh something like this.... { type buoyantPressure; rho rhok; value uniform 0; } see the tutorial on heatTransfer/buoyantBoussinesqSimpleFoam/ you will get an idea. 

June 6, 2013, 01:42 

#16 
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ankur
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Hey Tushar
I tried that also, but it didnt work. Another thing is that its totally forced convection and my gravity is also zero so buoyant does not mean anything here as I have understood. I do not know what else can go wrong in this simple problem. I will try more things now, lets see how it goes. You can also think what else can be wrong. Thanks 

June 6, 2013, 01:54 

#17 
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Tushar Chourushi
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Hello,
I mean to say by putting the mentioned BC for "p_rgh" and setting g=0, your case will be of forced convection only (i.e., independent of buoyancy). I have a doubt with pressure "p" BC. Try setting the BC for Outlet & inlet. Check: If you are not getting solution. Also check: Are you getting convergence? 

June 6, 2013, 02:19 

#18 
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ankur
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I am posting my p_rgh and U files, kindly suggest me what I should change,
P_rgh dimensions [0 2 2 0 0 0 0]; internalField uniform 0; boundaryField { inlet { type zeroGradient; } pipe { type zeroGradient; } outlet { type fixedValue; value uniform 0; } wall { type zeroGradient; } U dimensions [0 1 1 0 0 0 0]; internalField uniform (0 0 0); boundaryField { inlet { type fixedValue; value uniform (1 0 0); } pipe { type fixedValue; value uniform (0 0 0); } outlet { type zeroGradient; } wall { type fixedValue; value uniform (0 0 0); } I have tried changinp_rgh to buoyantPressure it was not converging. 

June 6, 2013, 02:45 

#20 
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ankur
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I changed the p_rgh to buoyantPressure and p file to zeroGradient at the inlet and fixedValue at the outlet.
It is showing this error > FOAM FATAL ERROR: Continuity error cannot be removed by adjusting the outflow. Please check the velocity boundary conditions and/or run potentialFoam to initialise the outflow. Total flux : 0.000771162 Specified mass inflow : 0.005 Specified mass outflow : 0 Adjustable mass outflow : 2.34371e110 From function adjustPhi(surfaceScalarField& phi, const volVectorField& U,const volScalarField& p in file cfdTools/general/adjustPhi/adjustPhi.C at line 118. FOAM exiting 

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