|
[Sponsors] |
Alletto - 2022 - Comparison of overset mesh with morphing mesh |
![]() |
|
LinkBack | Thread Tools | Search this Thread | Display Modes |
![]() |
![]() |
#21 |
New Member
Alvi Ahmmed
Join Date: Nov 2020
Posts: 7
Rep Power: 6 ![]() |
Thank you very much. I can get the natural frequency(fn) from St=fnD/U equation right? And am I free to choose U and D for a fixed Re=100?
|
|
![]() |
![]() |
![]() |
![]() |
#22 |
Senior Member
Michael Alletto
Join Date: Jun 2018
Location: Bremen
Posts: 616
Rep Power: 16 ![]() |
You can choose the parameters as you want as long all dimensional less parameters are the same. The frequency in the st number is the shedding frequency not the natural frequency
|
|
![]() |
![]() |
![]() |
![]() |
#23 |
New Member
Alvi Ahmmed
Join Date: Nov 2020
Posts: 7
Rep Power: 6 ![]() |
How can I find the value of natural frequency (fn) ? From the FFT plot of the lift coff? Regards.
|
|
![]() |
![]() |
![]() |
![]() |
#24 |
Senior Member
Michael Alletto
Join Date: Jun 2018
Location: Bremen
Posts: 616
Rep Power: 16 ![]() |
See https://en.m.wikipedia.org/wiki/Natural_frequency
For the natural frequency of a spring mass system. But I think I mentioned this also in the paper. Read it carefully. What is done in the python scripts is also explained in the paper. A fft of the lift signal is performed and the maximum amplitude is used to calculate the St number. Read the paper a few times if once is not enough. I usually need three or four times to fully understand a paper |
|
![]() |
![]() |
![]() |
![]() |
#25 |
New Member
Alvi Ahmmed
Join Date: Nov 2020
Posts: 7
Rep Power: 6 ![]() |
Thanks very much for your guidence
|
|
![]() |
![]() |
![]() |
![]() |
#26 |
New Member
Mehdi Badri
Join Date: Apr 2013
Posts: 7
Rep Power: 14 ![]() |
Hi,
According to the definition of non-dimensional mass, ![]() ![]() ![]() In your paper (and its corresponding git repo), you have used ![]() ![]() ![]() ![]() Could you please clarify how you calculated it (and why my understanding is perhaps incorrect)? |
|
![]() |
![]() |
![]() |
![]() |
#27 |
Senior Member
Michael Alletto
Join Date: Jun 2018
Location: Bremen
Posts: 616
Rep Power: 16 ![]() |
||
![]() |
![]() |
![]() |
![]() |
#28 | |
New Member
Mehdi Badri
Join Date: Apr 2013
Posts: 7
Rep Power: 14 ![]() |
Quote:
That is a nice explanation and helpful note! Thanks |
||
![]() |
![]() |
![]() |
![]() |
#29 |
Member
zink
Join Date: Oct 2015
Posts: 30
Rep Power: 11 ![]() |
||
![]() |
![]() |
![]() |
![]() |
#30 |
New Member
Wael Elorfi
Join Date: Feb 2022
Location: Egypt
Posts: 2
Rep Power: 0 ![]() |
Is there a bibtex file available for citing this paper?
|
|
![]() |
![]() |
![]() |
![]() |
#31 |
Senior Member
Michael Alletto
Join Date: Jun 2018
Location: Bremen
Posts: 616
Rep Power: 16 ![]() |
I usually copy the bibtex entry from Google scholar
|
|
![]() |
![]() |
![]() |
![]() |
#32 |
New Member
Wael Elorfi
Join Date: Feb 2022
Location: Egypt
Posts: 2
Rep Power: 0 ![]() |
Got it. Thanks a lot!
@article{alletto2022comparison, title={Comparison of overset mesh with morphing mesh: Flow over a forced oscillating and freely oscillating 2D cylinder}, author={Alletto, Michael}, journal={OpenFOAM{\textregistered} Journal}, volume={2}, pages={13--30}, year={2022} } |
|
![]() |
![]() |
![]() |
![]() |
#33 |
Senior Member
Håkan Nilsson
Join Date: Mar 2009
Location: Gothenburg, Sweden
Posts: 205
Rep Power: 19 ![]() |
This paper has now been updated with the ISSN of the journal and its own DOI: https://doi.org/10.51560/ofj.v2.47
|
|
![]() |
![]() |
![]() |
![]() |
#34 |
Member
zink
Join Date: Oct 2015
Posts: 30
Rep Power: 11 ![]() |
Hi,
Can anyone explain the m in this equation? Is it only the mass of the cylinder? Does this include the added mass as well? |
|
![]() |
![]() |
![]() |
![]() |
#35 |
Senior Member
Michael Alletto
Join Date: Jun 2018
Location: Bremen
Posts: 616
Rep Power: 16 ![]() |
It's only the mass of the cylinder
|
|
![]() |
![]() |
![]() |
![]() |
#36 |
Member
zink
Join Date: Oct 2015
Posts: 30
Rep Power: 11 ![]() |
I need some clarification regarding your paper
Q-1: You have mentioned that density of the cylinder is set to 14817 kg/mˆ3. It should be called as the density of the fluid not the cylinder? Q-2: In your calculations, in the case of Ur 4, you have used the k = m*(2*pi*f)ˆ2 that gives k value of 148.28. I want to ask about the f used in the calculation. We know that the reduced natural frequency of the system is given as Fr = I/Ur and Ur= Unif/f*D , here f is the frequency in the flow medium . It could be air, water or any medium used in the simulation. In the present case, it is the frequency in the fluid having density 14817 kg.m3. f= 0.0656/(4*0.0016) = 10.25 As you are using cylinder mass m=0.03575 ,then the k should be calculated as k=(m+m_added_mass)*(2*pi*f)ˆ2 m_added_mass= C_EA*(pi*Dˆ2*H*rhoInf/4) =0.003575 k=163.108 Please clarify? I just want to learn that how f is related with k when you are using medium other than air. Should it include the added mass or not? |
|
![]() |
![]() |
![]() |
![]() |
#37 |
Senior Member
Michael Alletto
Join Date: Jun 2018
Location: Bremen
Posts: 616
Rep Power: 16 ![]() |
Q1: It is the density of the cylinder. If you fix the mass and the dimensions of the cylinder the density can be calculated
Q2: The added mass is not considered. It is actually not known in advance since it is solution dependent. What did you mean with added mass exactly. Can you specify it more precisely? The purpose of setting the constants in the paper in the way I did it, is to match all relevant non-dimensional constants. This are U*, m* and Re. Actually you can choose all combination of dimensional quantities as you want as long as the non-dimensional quantities remain the same. If the non-dimensional quantities are the same you can compare the non-dimensional solutions. Have a look at the pi-theorem https://en.wikipedia.org/wiki/Buckingham_%CF%80_theorem Best Michael |
|
![]() |
![]() |
![]() |
![]() |
#38 | |
New Member
Manchester
Join Date: Aug 2022
Posts: 27
Rep Power: 4 ![]() |
Quote:
Many thanks for your contribution, one quick question is about overset mesh, for interpolation fringe, it's better to walk away from the cylinder boundary to avoid a huge gradient, is it right? When using overset mesh for your case, have you ever faced the issue at the interface between the overset component and background component? I mean the velocity and pressure field at this interface are not consistent, I think that's due to the issue about mass conservation, can we improve this phenomenon by adjusting the interpolation scheme? |
||
![]() |
![]() |
![]() |
![]() |
#39 |
Senior Member
Michael Alletto
Join Date: Jun 2018
Location: Bremen
Posts: 616
Rep Power: 16 ![]() |
Hello,
yes better avoid regions of strong gradients where to place the overset boundary. Best Michael |
|
![]() |
![]() |
![]() |
![]() |
#40 | |
New Member
Manchester
Join Date: Aug 2022
Posts: 27
Rep Power: 4 ![]() |
Quote:
Thank you for your sharing, which helps me a lot. I noticed you used cubic for div(phi, U) term instead of other second-order discretization schemes. I tried linearUpwind, QUICK, and cubic, and the results changed a lot, actually for the overset mesh, linearUpind predicts the highest frequency of lift coefficient, but the cubic returns the highest amplitude and reasonable frequency. Can you please explain why, is there any useful reference to support it? Best, Tian |
||
![]() |
![]() |
![]() |
Thread Tools | Search this Thread |
Display Modes | |
|
|
![]() |
||||
Thread | Thread Starter | Forum | Replies | Last Post |
[snappyHexMesh] SnappyHexMesh/splitMeshRegion : region1 in zone "-1" | GuiMagyar | OpenFOAM Meshing & Mesh Conversion | 3 | August 4, 2023 12:38 |
objects oscillate at high speed causing collapse in Dynamic mesh and overset mesh ca | insane | OpenFOAM Running, Solving & CFD | 0 | May 17, 2020 22:35 |
Overset: refine background mesh without resetting the mesh | JohnAB | STAR-CCM+ | 6 | May 19, 2014 13:48 |
Help in setting up an overset mesh | RKE | STAR-CCM+ | 1 | February 21, 2014 21:35 |
Icemcfd 11: Loss of mesh from surface mesh option? | Joe | CFX | 2 | March 26, 2007 18:10 |