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August 28, 2018, 14:48 |
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#21 | ||
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Thank you for the list. I quickly glanced over the first manuscript - it does state that Quote:
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August 28, 2018, 15:53 |
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#22 | |
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Filippo Maria Denaro
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The definition of a "perfect model" strictly depends on the definition of the LES filter. In case you apply an explicit filtering procedure, you can really have a congruent coupling with the DNS (filtered) fields. On the other hand, the common use of an implicit filtering makes more complicated to define the correct unresolved field and insert into LES. What is intriguing is the RANS is based on a well defined statistical averaging and the "perfect model" should be well suited. |
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August 28, 2018, 16:09 |
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#23 | ||
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August 28, 2018, 16:11 |
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#24 |
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From DNS you could compute the "exact" unresolved terms to be included in a steady RANS, so I don't see a theoretical reason for which it can not work....
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August 28, 2018, 16:22 |
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#25 | |
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b) how to discretize tau, i.e. how to apply die divergence operatot consistently. If one of the two steps is not done correctly, the solution of the DNS and the perfect RANS should differ. |
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August 28, 2018, 16:30 |
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#26 | |
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Filippo Maria Denaro
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You could compute div Tau directly on the DNS grid so that you have a fully resolved and accurate term to be inserted into the RANS solver. |
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August 28, 2018, 16:37 |
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#27 |
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Then div tau would be exact - but shouldnt the divergence operator be the discrete one then? The one on the left side is. For the terms in tau and the convective term to cancel (otherwise the solution to the equation is no linger the filtered DNS), not only the terms themselves must match, but also their discretizations.
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August 28, 2018, 16:41 |
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#28 | |
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Filippo Maria Denaro
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You could also think to solve the RANS over the DNS grid, just a 2D plane of the DNS grid is sufficient. I don't see a theoretical reason to not get a convergence. |
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August 28, 2018, 16:50 |
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#29 | |
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I think I have to disagree - from the paper they solve the equations on the RANS grid, and then averaging / filtering and discretization errors mingle. It is possible to account for that (this is why in the paper you cited, the LES is filtered explicitly and the equations are solved on a fine grid), but it is unclear / not mentioned in the paper. I find it curious that they note the discrepancy fir increasing Re on a fixed grid - this is exactly what would happen as a consequence of what I have outlined here. |
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August 29, 2018, 05:23 |
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#30 | |
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Dear FMDenaro, having gone through the literature you provided and others, I found that the picture is different for RANS than it is for LES. For LES, the general observation is that inserting the closure from DNS works - as one would expect from a mathematical point of view. For RANS, the picture is not so clear, there might be something going on there. So for RANS, this would pose a problem for ML methods, while not for LES. Thanks again for providing these insightful literature links! |
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August 29, 2018, 05:27 |
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#31 | |
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LES might be forgiving because the unsteady term can accomodate anything unbalanced. In contrast, RANS can't; moreover, it also needs that the equilibrium found among all the terms is actually stable (which seems to be the real issue here, if I read correctly some of the material you all posted here). |
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August 29, 2018, 05:48 |
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#32 | |
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August 29, 2018, 05:54 |
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#33 | |
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August 29, 2018, 05:56 |
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#34 | |
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No, but if - like in the paper I posted - the filtered equations are started from a filtered DNS and then evolved with the closure terms (derived by filtering the DNS), then these two quantities are and remain identical (within rounding error limits). |
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August 29, 2018, 05:57 |
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#35 | |
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August 29, 2018, 05:59 |
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#36 |
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The problem is 1) identify the LES filter to use on DNS. 2) using the LES equations with the perfect model but on the DNS grid or not?
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August 29, 2018, 06:01 |
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#37 | |
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"We demonstrate, in the context of implicit-filtering large eddy simulations (LESs) of geostrophic turbulence, that while the attractor of a well-resolved statistically stationary turbulent flow can be reached in a coarsely resolved LES that is forced by the subgrid scale (SGS) terms diagnosed from the well-resolved computation, the attractor is generically unstable: the coarsely resolved LES system forced by the diagnosed SGS eddy terms has multiple attractors. This points to the importance of interpreting the diagnosed SGS forcing terms in a well-resolved computation or experiment from a combined physical-numerical point of view rather than from a purely physical point of view." As I remember of different works actually trying this (not only these 2), it may actually depends from the specific details of the implementation (as, btw, it is typically the case in LES). |
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August 29, 2018, 06:06 |
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#38 | |
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August 29, 2018, 06:11 |
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#39 | |
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1) What is done in two papers I mentioned is independent of the filter used on the DNS - it clearly gives a different solution u_filtered, but the overall perfect LES is independent of that. 2) In both publications, the perfect LES is actually solved on the LES grid, so discretization errors have to be balanced out by a term in the closure, see EQ 6 in the Nadiga paper. |
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August 29, 2018, 06:16 |
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#40 | |
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Ok, I understand how this summary might be misinterpreted. What they are doing in the paper is: a) show that with the filtered DNS as a closure, the solution remains the filtered solution for all times. BTW, this is also shown in the paper about the ML I mentioned earlier that somewhat started this discussion. b) They then perturb the closure term and observe a deviation. Here is the Fig. 1 from the paper I was talking about https://ibb.co/jx9O59 This last point is what they refer to in their summary. |
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