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Divergence for compressible flow with rough walls |
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September 16, 2022, 12:32 |
Divergence for compressible flow with rough walls
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#1 |
New Member
Jannis
Join Date: Sep 2022
Posts: 7
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Hello everyone,
I'm currently doing a heat-transfer analysis an a nozzle with compressible flow with the k-w-SST turbulence model. Therefore I want to include rough walls with a roughness height of 129µm. But as soon as I include them, my solutions never converge and I get extreme values in the boundary layer. An inflation layer with an initial first cell height of 5,67e-3mm is included, but I also tried lower and larger values. I'm running the pressure-based solver since I never got the solution to converge with density-based. Other settings are coupled scheme, second order discretization, pseudo transient. But I also tried other inputs also for the relaxation factors, which are currently set to default. I included a photo for rough walls and for smooth walls, all other settings are the same for both simulations. With lower roughness heights (20µm) I reached convergence and plausible results. If anybody has a guess on what might cause the divergence and extreme values I would be happy to here them. Thanks Jannis Mach_roughwalls.jpg Mach_smoothwalls.jpg Last edited by turbvisc; September 16, 2022 at 14:08. |
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September 20, 2022, 05:22 |
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#2 |
Senior Member
Alexander
Join Date: Apr 2013
Posts: 2,363
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roughness height of 129µm is bigger than initial first cell height of 5,67e-3mm
however, lower roughness heights (20µm) is bigger either I would check this first also you may try to simulate in transient to get better convergence
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September 20, 2022, 15:26 |
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#3 |
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Lucky
Join Date: Apr 2011
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Most likely a general convergence error not really related to roughness. The roughness height just modifies slightly the wall shear stress. Just try to find a more robust approach or figure out where it is diverging (it's almost always where the shitty cells are).
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September 23, 2022, 10:22 |
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#4 |
New Member
Jannis
Join Date: Sep 2022
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Thanks to both of you for your input. Sadly the advice you gave didn't really make a different in my calculations.
On thing that did work however was to use the high roughness (icing) model for the wall roughness. I get converged and plausible values using that approach. |
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September 23, 2022, 12:18 |
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#5 |
Senior Member
Lucky
Join Date: Apr 2011
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Icing in a rocket nozzle is a plausible result? Well okay then
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September 23, 2022, 12:32 |
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#6 |
New Member
Jannis
Join Date: Sep 2022
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Well Icing isn't, but the model is, even though primarily, not exclusively for Icing simulations, but also for high roughness walls.
high_roughness.png |
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September 23, 2022, 17:38 |
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#7 |
Senior Member
Lucky
Join Date: Apr 2011
Location: Orlando, FL USA
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Well I've never seen a rocket with rough walls either so there's that.
The expression grasping as straws comes to mind. Look, you got unlucky with your original settings and kept clicking buttons until something did work. Tomorrow you'll run a flat plate and it may or may not converge. And one day you'll run a pipe and it may or may not work. You'll continue to have these experiences until you figure out what makes stuff diverge in the first place and I'll tell you, it isn't wall roughness because you can simply turn off the wall roughness altogether by making it a slip wall. |
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September 24, 2022, 13:41 |
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#8 |
New Member
Jannis
Join Date: Sep 2022
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It's additively manufactured, hence the roughness.
I ran it with smooth walls, it converged. I ran it with lower roughness values, it converged. I also ran it with an other turbulence model (k-epsilon) and it did also converge. Just the combination of k-w and the high roughness gave problems. So I tried to understand how the roughness is taken into account by the turbulence model and stumbled over the high roughness model for the SST model in the theory guide, which uses a different modelling for k and w near the wall, which was the region where problems occurred, and why I tried it out. Is that such bad of a practice? |
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Tags |
compressible, divergence, rough wall, roughness |
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