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Turbulent Boundary condition, viscosity ratio and length scale |
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October 17, 2012, 04:31 |
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#21 |
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Francisco
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You are right, my Re no is 40.4 times higher. Should I try with a finer mesh so? I'm considering to reduce scale to get a similar case to the one in the reference and compare results. And once then go back to the current scale.
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October 17, 2012, 04:38 |
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#22 |
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Philipp
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Just reduce your inlet velocity by a factor of 40 and give it a try. If you don't have any problems then, you know that your grid needs some refinement for your current case. (Don't forget to enlarge the timestep, when you reduce the velocity)
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October 17, 2012, 16:30 |
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#23 |
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Francisco
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Well, I’ve run the case for 0.25 m/s, using the same solver setup and different time steps: 1, 2 and 4 s. Convergence criteria 1e6 as before.
I comment a few things: 1) Almost no TVR limitation, just a few cells (small vortexs) at some iterations. 2) Y+ very small, from 0.1 to 1.8. First layer of prism layer should be higher for SWF. (see picture) 3) Epsilon residuals in some iterations can’t go under 1e6. 4) Turbulence intensity drops too fast so close to the inlet. (see picture) I’ve read in the forum that if TI drops too much it means that equilibrium between k and e is wrong because I have too much dissipation, e is over estimated. I guess I need a higher amount of TI in the inlet so I get the desired value at the plate? But if I put too much TI and initialize the solution from the inlet it may start with TVR limitation from the beginning. 5) Lift and drag keep oscillating even if I have left time enough for the flow to run the entire domain for twice (3200s at 0.25 m/s) (see pictures) I’m gonna try to simulate at the same scale as the reference, with same Re number and try to get a correct y+ value. Once then I'll have to try again the real scale. Any suggestions? Thanks a lot |
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October 18, 2012, 03:39 |
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#24 |
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Philipp
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Hey,
2) With an y+ of that size: If you can afford that mesh (by means of computational power) you can just use the "enhanced wall treatment" instead of wall functions. 4) I don't know much about that, but what you write sounds reasonable. You say, that TE drops on the way from your inlet to your plate, correct? Now, shouldn't you fix your k and e at the inlet in a way, that the 10% TI is sustained? Or isn't that possible? 5) Your plate has a much higher angle than in the paper, right? Isn't it possible that lift and drag are strongly time dependent? Looks like you have strong oscillations in the wake... |
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October 18, 2012, 04:00 |
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#25 |
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Sorry I was busy for 2 days, I worked on your geometry and I guess I got the good blocking.min quality is 0.8 which is very good but you have to work yourself on the edge parameters and refine/coarsen the mesh in the appropriate areas and finally put BC's and export the mesh in fluent. I am attaching few pics and project files of ICEM
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October 18, 2012, 04:07 |
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#26 | |
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One more suggestion...use SST kw model instead of k-epsilon because angle of attack in your case is very high and there is significant amount of flow separation and k-epsilon model does not properly capture separation instead SST kw model is more recommended in such a situation. Another point....if turbulent viscosity limit is exceeding in few cells then you don't need to worry as long as your lift and drag are in agreement with experimental results Regards |
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October 18, 2012, 08:29 |
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#27 |
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Francisco
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@cfdseeker Thank you very match for the files! That will help me a lot to learn more about ICEM.
As this case has a clear separation point at the edge of the plate, is there a big diference between k-e and k-omega? @rodrigeuzfatz @cfdseeker I've run the case at a smaller scale and almost didn't have any TVR limitations, just few cells away from the plate at some iterations, nothing to worry about. y+ is still too low, I prefer to coarsen my inflation layer and use a wall function instead of using the enhanced wall treatment in order to reduce computational effort. Force coefficients don't oscillate as much as they did before, they are still a bit higher than in literature but I guess I have to resolve near wall flux properly before. I've read something about TI decay in Fluent users guide (7.2.2), there are some equations to estimate k and e from TI decay and distance. Is there a way to get time-averaged variables along the plate wall? The only way I know to do that is to write an xy-plot file for each time, and then calculate the mean value. However, I need to save many .dat files to have a good resolution. I'll share further results. Regards. |
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October 18, 2012, 12:28 |
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#28 | ||
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Quote:
Quote:
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October 19, 2012, 04:34 |
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#29 |
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Francisco
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Okay, I'll try SST k-w model with the finner mesh, the thing is y+ distribution around the plate reaches very different values. There's always a minimum at the stagnation point in the front face and at two corners but there are peaks at the back face and the two other corners that goes over 1 in the finner case (see y+ picture at comment #23)
1) Do I have to get y+<=1 along all the wall? as the case is strongly time dependent, do I have to look at time-averaged y+ or just the maximum? By the way, these guys get very good results for a vertical plate in the same conditions as me (just a little geometry difference) using k-e with different wall treatments and they don't use a prism layer around the wall. http://www.waset.org/journals/waset/v61/v61-49.pdf 2) What are they doing that I'm missing? |
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October 19, 2012, 08:48 |
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#30 |
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Francisco
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I've run the case with SST k-w model, no TVR limitations appeared. The problem is I'm still having wrong force coeficients. Time averaged values are the same as in all previous simulations: Cd=2.979 and Cl=-1.071 while literature ones are Cd=1.945 and Cl=-0.708.
I've been looking at Cp distribution at the plate and made the time average over a complete vortex sheddind cycle. I've compared it to literature values and my Cp's at the back face are much lower (see attached pictures), that's why my Cd and Cl are higher. So I must be simulating something wrong at the wake, could it be because of wrong y+ values at the back face? (see picture of instantaneous y+ at Cd max time) What can be the reason for too low pressure at the back face? Thanks a lot for your help guys |
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October 20, 2012, 04:37 |
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#31 | ||
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October 20, 2012, 04:39 |
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#32 | |
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October 20, 2012, 09:28 |
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#33 |
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Francisco
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I'm not pretty sure if transition is taking place. How can I asure that the case is fully turbulent?
I've increased TI from 10% to 25% at the inlet and let the same turbulent lenght scale (TLS) of 9e-4 m and results are the same. Now I'm running a case with 25% of TI at the inlet but a TLS of 5e-5 m to make it more diffusive to see if something changes. |
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October 20, 2012, 12:14 |
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#34 | |
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Quote:
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October 20, 2012, 12:40 |
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#35 | |
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Quote:
1. Reynolds number 2. Time step and no of time steps and how you have determined them? 3. How you are making the time-average Cd and Cl. How many time steps and total time you are taking into account for this purpose? 4. How you are ensuring the convergence 5. Domain extent is good enough? Have you made the sensitivity analysis to domain extent? |
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October 20, 2012, 12:54 |
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#36 | |
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Francisco
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Hi far,
I've already solved TVR limitations by scaling the problem and using a better turbulence lenght. k-e standar with standar wall function and k-w with enhanced wall treatment are not showing this limitation. The problem is both models give too low pressure at the near wake and so drag and lift coeficients are higer than they should be. I'm now playing with BC for TI(%) and T length scale to see if results change, but force over the plate is not changing so far. I think it may be related to turbulence model or its parameters. Quote:
Thanks |
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October 20, 2012, 13:15 |
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#38 |
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Francisco
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I've just seen your last comment.
1) Re no is 1.55e5 (plate length=0.15m, u=15m/s) 2) I've tried several timesteps: 5e-4, 1e-3, 2e-3 and eventually I'm using 25e-4. I let the flow goes several times all along the domain (6.25 m long) that is 800 timesteps. But I've have checked that mroe iterations don't change the result. 3) Once the coefficients are constante I've measured the period of a cycle of lift and drag force, they are almost 0.07s and I've writen a Cp file every 0.001s. I've made the average for each point and got the time-averaged Cp distribution for a complete cycle. 4) Residuals are 1e-5. 5) Now it's 41.6*L long and 27.7*L where L is the plate length 015m. I've tried a larger one and results are the same. 3) |
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October 20, 2012, 13:45 |
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#39 |
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Francisco
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By scaling I mean to reduce the scale of the mesh.
My real plate is 9.13m but I wanted to compare with literature experiments for a 0.15m plate. So I reduced mine to have the same length. The real scale problem gave TVR limitation but the same mesh with reduced scale gave no problem. |
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October 20, 2012, 14:00 |
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#40 |
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What is the value of density and viscosity and why you choose these values?
How did you determine the time step size? Is it according to any method available in literature? Do you wanna try the hexa mesh? I have made one. In this mesh, Y+ is 1 (good for transition model as well) but requires more time steps. You may need the transition model for better prediction of Cd. |
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3d 2d, flat plate, turbulence models, viscosity limitation |
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