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Old   July 12, 2011, 11:31
Default How about dynamic Smagorinsky?
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Bernhard
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Hi all,

I have some questions about this same issue with respect to the dynamic Smagorinsky model. I think I am making a mistake somewhere, but please correct me if I am wrong. I've tried to look at other locations for the same issue, but couldn't find it.

I compare the dynamic model in OpenFOAM (not caring about the domain averages coefficient) with the dynamic model (described in Lilly and Pope).

I think we agree on the following (D defined in OpenFOAM, S common definition)
\begin{array}{rcl}
\overline{S}_{ij} &=& \frac{1}{2}\left(\frac{\partial u_i}{\partial x_j}+\frac{\partial u_j}{\partial x_i}\right) \\
\overline{D}_{ij} &=& \overline{S}_{ij} - \frac{1}{3} \delta_{ij}\overline{S}_{kk} = \overline{S}_{ij} (incompressible) \\
|\overline{D}| &=& |\overline{S}|/\sqrt{2}
\end{array}

Now, looking at the code (dynSmagorinsky 1.7, homogeneousDynSmagorinsky 2.0), in the .C file at line 57, 62 respectively:
M_{ij} = \Delta^2 \left[ \widehat{|\overline{D}|\overline{D}_{ij}} - 4 |\widehat{\overline{D}}_{ij}\widehat{\overline{D}}_{ij}|\right]
as compared to the original of Lilly (in Pope this expression
M_{ij} = \widehat{\Delta}^2\widehat{|\overline{S}|}\widehat{\overline{S}}_{ij}-\Delta^2\widehat{|\overline{S}|\overline{S}_{ij}}

If D_ij=S_ij, but |S|=sqrt(2) |D|, then the second term in the OF implementation is off by a factor sqrt(2). (Where the factor 4 is from the double width of the test filter, and the minus sine is also present in L)

Somewhere I must have skipped a step, I hope one of you can point it out for me. Thanks in advance!
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Old   July 15, 2011, 02:35
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Anybody that can give a comment on this?
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Old   July 18, 2011, 03:47
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Mistake is this:
Quote:
Originally Posted by Bernhard View Post
M_{ij} = \Delta^2 \left[ \widehat{|\overline{D}|\overline{D}_{ij}} - 4 |\widehat{\overline{D}}_{ij}\widehat{\overline{D}}_{ij}|\right]
M_{ij} = \Delta^2 \left[ \widehat{|\overline{D}|\overline{D}_{ij}} - 4  |\widehat{\overline{D}}|\widehat{\overline{D}}_{ij}\right]
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Old   August 26, 2011, 06:39
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Quote:
Originally Posted by lakeat View Post
Question 1: Why using magSqr(dev(symm(gradU))) instead of symm(gradU) && symm(gradU) to get {{\bf{\bar S}}{\rm{:}}{\bf{\bar S}}} ????
Thank you
I think the reason is to have a consistent formulation for incompressible an compressible LES models :

let symm(gradU) be S, then dev(S) = S - 1/3 trace(S)I

however in a incompressible case
1/3 trace(S)I = 0, since trace(S) is the continuity eq. . Therefore in an incrompessible case it doesnt matter whether you take dev(S) or not , but consider a compressible case then 1/3 trace(S) doesn't vanish.

In a compressible or variable density case the solver calls divDevRhoBeff to compute the source term due to SGS stress B = 2/3k I - 2 nu_t S_D. (See Fureby http://pof.aip.org/resource/1/phfle6/v9/i5/p1416_s1 Eq. 3) There you have the deviatoric part of D. But i guess openFoam uses nu_t = c Delta^2 ||S_D|| and B = 2/3k I - 2 nu_t S. So it takes S_D for the turbulent viscosity and S for the SGS stress tensor B.
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Old   January 24, 2013, 10:40
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Quote:
Originally Posted by MaximeIST View Post
Hello

I may keep on confusing people, but the way it is coded, if I am not doing mistake is
Cs=sqrt(ck*sqrt(2*ck/ce))
in the incompressible Smagorinsky.H line 114.
There is a factor 2 added in the root-mean squared.

And in the case where Ce=1.048 and Ck=0.094, and with this factor 2, we obtain Cs=0.1995.

May be I miss something?

Maxime
Hi All,

For the compressible Smagorinsky model, the parameters for ck=0.02, ce=1.048

Following the following line:
Cs=sqrt(ck*sqrt(ck/ce))
=> Cs=0.0525...

Does anybody know the references for these specification of the ck and ce for compressible Smagorinsky model?
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Old   March 11, 2013, 21:25
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Hi Yingkun,

As you mentioned, in the incompressible solvers Cs=sqrt(Ck*sqrt(Ck/Ce)). So if I want to set Cs=1, Do I just need to modify Ck and Ce in the LESProperties?Or are there other rules I must obey?
Code:
SmagorinskyCoeffs
{
ce 1.05;
ck 0.0472;
}
regards
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Old   February 28, 2014, 03:03
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Hi Bernhard and everybody,

I compare the dynamic model in OpenFOAM (homoDynSmag OF 2.2.2) with the dynamic model (described in Lilly and Pope) and I have the same Problem. To reanimate the discussion:

In Pope (F(.) means filtered):
[1] nu_SGS = cS * delta^2 * sqrt(2 * S_ij S_ij)
[2] cs = (M_ij L_ij)/(M_kl M_kl)
where
[3] S_ij = 0.5 (ui,j + uj,i)

[4] M_ij = 2 * delta^2 * (F(sqrt(2 * S_ij S_ij) S_ij) - F(sqrt(2 * S_ij S_ij)) F(S_ij))
[5] L_ij = F(ui uj) - F(ui) F(uj)

In OF 2.2.2 (homogeneousDySmagorinsky, <.> means averaged):
[6] nu_SGS = cD * delta^2 *
sqrt(S_ij S_ij)
[7] cD = 0.5 (<L_ij M_ij>)/(<M_kl M_kl>)
[8] S_ij = D_ij = S_ij Pope
[9] M_ij = delta^2 * (F(sqrt(S_kl S_kl) Sij) - 4 * sqrt(<S_kl> <S_kl>) <S_ij>)
[10]
L_ij = F(ui uj) - F(ui) F(uj)


I marked the differences of these models.

- First difference is the factor 0.5 in Eq[7] in comparison to Eq[2]. This comes from the factor 2 in Eq[4]. If we put this in Eq[2] we get 0.5 (ok)


- Second difference is the different filtering in M_ij. What effect does this have???? (x)

- Third difference is the factor 4 in Eq[9] in comparison to Eq[4]. Bernhard:

here the factor 4 is from the double width of the test filter
can you please explain that?? Why we don`t get a fector in the other filtered terms??? (x)

- Fourth difference is the factor 2 in mag(S_ij). (x)

In my opinion these models are different or I`m not able to bring the OF-model in the form of pope-model.
If it is possible, anyone can please give some advice?


kind regards
Florian
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Old   October 28, 2014, 01:39
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Quote:
Originally Posted by lakeat View Post
Sorry, I do not understand, I saw in "Smagorinsky.H",
Code:
tmp<volScalarField> k(const tmp<volTensorField>& gradU) const
{
    return (2.0*ck_/ce_)*sqr(delta())*magSqr(dev(symm(gradU)));
}
As I remember:

\begin{array}{l}
 {\nu _{SGS}} = {\left( {{C_S}\Delta } \right)^2}\left| {{\bf{\bar S}}} \right| \\ 
 K = {\left( {{C_I}\Delta } \right)^2}{\left| {{\bf{\bar S}}} \right|^2} \\ 
 \left| {{\bf{\bar S}}} \right| = {\left( {{\bf{\bar S}}{\rm{:}}{\bf{\bar S}}} \right)^{{1 \mathord{\left/
 {\vphantom {1 2}} \right.
 \kern-\nulldelimiterspace} 2}}} \\ 
 \end{array}





Question 1: Why using magSqr(dev(symm(gradU))) instead of symm(gradU) && symm(gradU) to get {{\bf{\bar S}}{\rm{:}}{\bf{\bar S}}} ????

Question 2: If magSqr(dev(symm(gradU))) = symm(gradU) && symm(gradU) = {{\bf{\bar S}}{\rm{:}}{\bf{\bar S}}}, then

K = \frac{{2{C_K}}}{{{C_\varepsilon }}}{\Delta ^2}{\left| {{\bf{\bar S}}} \right|^2}

But I saw in "Smagorinsky.C"
Code:
nuSgs_ = ck_*delta()*sqrt(k(gradU));
Which means

{\nu _{SGS}} = {C_K}\Delta \sqrt K

Then, replace K with K = \frac{{2{C_K}}}{{{C_\varepsilon }}}{\Delta ^2}{\left| {{\bf{\bar S}}} \right|^2}

{\nu _{SGS}} = {C_K}\Delta \sqrt K  = {C_K}\Delta \sqrt {\frac{{2{C_K}}}{{{C_\varepsilon }}}{\Delta ^2}{{\left| {{\bf{\bar S}}} \right|}^2}}  = {C_K}\sqrt {\frac{{2{C_K}}}{{{C_\varepsilon }}}} {\Delta ^2}\left| {{\bf{\bar S}}} \right|


Compare with {\nu _{SGS}} = {\left( {{C_S}\Delta } \right)^2}\left| {{\bf{\bar S}}} \right|

We'll get

{\left( {{C_S}} \right)^2} = {C_K}\sqrt {\frac{{2{C_K}}}{{{C_\varepsilon }}}}

But I heard somone said {\left( {{C_S}} \right)^2} = {C_K}\sqrt {\frac{{{C_K}}}{{{C_\varepsilon }}}}

So, I'm puzzled, I wonder if it was a mistake, that k should be written as
Code:
tmp<volScalarField> k(const tmp<volTensorField>& gradU) const
{
    return (ck_/ce_)*sqr(delta())*magSqr(dev(symm(gradU)));
}
Thank you


\begin{array}{l}
 {\nu _{SGS}} = {\left( {{C_S}\Delta } \right)^2}\left| {{\bf{\bar S}}} \right| \\ 
 K = {\left( {{C_I}\Delta } \right)^2}{\left| {{\bf{\bar S}}} \right|^2} \\ 
 \left| {{\bf{\bar S}}} \right| = {\left( {{\bf{\bar S}}{\rm{:}}{\bf{\bar S}}} \right)^{{1 \mathord{\left/
 {\vphantom {1 2}} \right.
 \kern-\nulldelimiterspace} 2}}} \\ 
 \end{array}

the third one shoub be sqrt(2*Sij*Sij)
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Old   December 11, 2014, 05:40
Default How to change ck and ce in Smagorinsky approach
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Greetings All

I have performed a Smagorinsky-based compressible LES simulation with the Coefficients as follows:

HTML Code:
{
  ce = 1.048;
  ck= 0.02;
}
According to the relation:

{\left( {{C_S}} \right)^2} = {C_K}\sqrt {\frac{{{C_K}}}{{{C_\varepsilon}}}}

I will get C_S= 0.053.
My case is a reacting non-premixed combustion with a bluff-body separating fuel and oxidizer streams.

I want to change the C_S value into 0.13. which value between C_K and C_\varepsilon should be modified to retain the nature of the problem?

Best,
Bobi




Last edited by babakflame; December 11, 2014 at 06:45.
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Old   March 21, 2015, 18:27
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Actually in this paper, we cannot find the information about how the model constants c_k=0.094 and c_{\epsilon}=1.048 come out. So which one is correct reference when I use these two constants? Thanks.

Quote:
Originally Posted by alberto View Post
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Old   September 21, 2015, 10:11
Default Openfoam
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Hi Lakeat,now I want to write the Scalar SikSkj,but how to write that in openFoam, Thanks.
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Old   January 15, 2016, 12:56
Default Change the smagorinsky coeff
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Elyas_Kermani
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hi friends
How can I change the smagorinsky Coeff (Cs) in OF?I want to use Cs=0.1...
Regard
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Old   December 26, 2017, 21:16
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I read that all the previous posts and reply.

May I understand that Cs=sqrt(Ck*sqrt(2Ck/Ce)) is correct in OpenFoam?


Thanks a lot
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Old   March 26, 2019, 05:15
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dear madam
As you know the smagorinsky constant Cs in OpenFOAM is defined as a function of Ce and Ck. But when i do the simulation for various combinations of Ck and Ce, that gives the same Cs, I am getting different results. So could you please tell Me where else Ck and Ce is used other than in smagorinsky model. My problem is incompressible LES with standard smagorinsky model and vandriest delta.

please help


my mailId is manafaero@gmail.com
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Old   March 31, 2019, 15:24
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Quote:
Originally Posted by manafaero View Post
But when i do the simulation for various combinations of Ck and Ce, that gives the same Cs, I am getting different results. So could you please tell Me where else Ck and Ce is used other than in smagorinsky model.
The nut, k and epsilon fields are created by these classes, but I 'm not familiar with LES modelling. Either way, if you look for "Ce_" and "Ck_" in those files, you will see how they are used.
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Old   April 3, 2019, 08:54
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I would like to share some experience of mine regarding the discussion. I also verified the equations given in the discussion. But when i run the simulation for various ck and ce combinations I am getting different results. the nu sgs is not the same in all cases. so eventhough the formula is correct the openFoam is not calculating as per the discussion. Note that I had removed the dependence of k in calculating shear stress B. but still the results differ. So be careful before using this. Also I am a beginner to OpenFOAM and C++. If any body is interested and any comments please post. my mail ID is manafaero@gmail.com.
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Old   September 16, 2020, 11:30
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did you check this page with OF implementation https://caefn.com/openfoam/smagorinsky-sgs-model
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