Issues with 'cmue_a'

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Boqi Boqitian@UW.Edu

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Aug 27, 2025, 5:34:08 PMAug 27
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Hi Lars, Hans and GOTM,


We are trying to integrate the “non-local, exact weak-equilibrium stability function” (after Gibson and Launder, 1976, per GOTM manual) into another model nonlocal with another closure we have been working on that accounts for some pressure-strain terms near boundaries. 


When we look at corresponding source code 'cmue_a.F90' we see it's in a “testing stage”, apparently since 2005. 


We note a sequence of two lines where the second overrides the first, which is more faithful

        Nt   =   0.5*(Pe-1.) + ct1 + 0.5*r_i*(Pbeb - 1.) ! general

        Nt   =   (Pe-1.) + ct1                           ! weak equilibrium


We also note there is no constraint related to realizability or stability in cmue_a as there is e.g. in the weak equilibrium (cmue_c) or quasi-equilibrium (cmue_d) code.


Can anyone recall and relate experience working with cmue_a two decades ago? Was there any conceptual or numerical problem in particular that hindered carrying this integration into GOTM forward, or are we reading too much in between those contradictory lines of code?


Is anyone else currently working on this? Perhaps in follow-on to Legay, Deremble & Burchard (2025:  https://doi.org/10.1029/JC095iC09p16179 )?


Thanks.


Regards,

Kevin Tian & Ramsey Harcourt

University of Washington


Lars Umlauf

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Aug 28, 2025, 3:32:05 AMAug 28
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Hi Kevin and Ramsey,

As far as I know, nobody has really worked on these parts of the code since I've implemented them into GOTM many years ago. Hans and I basically never found the time to follow up on this because other things came up.  

As shown by Legay et al. (2005), including this non-local framework in closure models improves the surface-layer structure especially during convection, and I am convinced this also applies to other non-local processes like LT. So it is really great that you're working on this type of models. I hope we can talk about this at the WTD.

All the best,

Lars

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Helmut Z. Baumert

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Aug 29, 2025, 11:22:03 AMAug 29
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Hello folks and namely Kevin, Ramsey and Lars,

attached please find an older paper where the physical background of
turbulence modeling is discussed at Re=\infty. It gave reasonable
ANALYTIC results for a number of well-known universal constants, e.g.
for von Karman's constant as 1/SQRT(2\pi)=0,398 ...~ 0,40.

Also other constants like pre-factors of the Kolmogoroff's frequency and
wave-number spectra are given, close to the observed/measured values in
super-pipes.

I remember that a plausible value for c_mue as
1/\pi_squared ~ 0,101... resulted from that theory, but was not yet
included in the attached paper due to other obligations. If you will
approach the problem in students's PhD theses, please let me know ...

Best regards,
Helmut Z. Baumert
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Univ_May_2013.pdf
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