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-   -   Variable Density - Free Surface with FIDAP (http://www.cfd-online.com/Forums/fluent/27613-variable-density-free-surface-fidap.html)

Vitaliy Pavlyk April 6, 2000 07:34

Variable Density - Free Surface with FIDAP
 
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I use FIDAP 8.52 to study weld pools. A weld pool is essentially a FREE-Surface system. FIDAP works quite well in almost all aspects of the phenomena involved (Marangoni, buoyancy, electromagnetic body force, phase change etc.)


But there is a problem with the volume expansion caused by the phase change and heating.


In order to illustrate the question
, consider a glass of water, which is totally full. When we heat the bottom of the glass, the water expands, the deformed free surface is the result (a sketch is given below). The above situation is considered as a TRANSIENT, COMPRESSIBLE(VARIABLE-DENSITY), FREE problem, the density being a function of temperature (expressed through a volume expansion coefficient).


It seems, that FIDAP fails to represent correctly the pressure gradient caused by density variations due to the heating. Instead, zero pressure results, if the problem is specified as COMPRESSIBLE(Variable-Density) <U>and</U> FREE.

However, if the outlet is fixed in space (like an outlet from a pipe) and the problem is NOT specified as FREE, but is still COMPRESSIBLE, the pressure is correct, and the amount of fluid passed across the outlet in course of reaching the steady-state satisfies the mass balance within a tolerance of 0.01 % !

The segregated solver with pressure-projection algorithm and kinematic update of the free surface is used.


I guess, <U>there is a defect in FIDAP</U>, when COMPRESSIBLE and FREE keywords are specified simultaneously.

Any other ideas how to model the "water expanding from a glass"?


Thank a lot,


Vitaliy.


__ Sketch of the problem (the gravity is zero for simplicity) :
</FONT><FONT FACE="Courier New" SIZE=2>

************wall (no-slip)

***********_______________

Time=0*:**</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>****************

**********</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>**************** <- outlet

bottom -> </FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>**************** (free surface)

heat flux </FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>**************** T=const

(constant)</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>_______________*

*************symmetry


Time > 0 :*_______________

**********</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>***************.*

**********</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>***************.**

**********</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>***************.***

**********</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>***************.****

**********</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>___________________*


Time-> <FONT FACE="Symbol"></FONT>

(steady-state):

***********_______________

**********</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>***************.**

**********</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>***************.****

**********</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>***************.******

**********</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>***************.*******

**********</FONT><FONT FACE="Symbol" SIZE=2></FONT><FONT FACE="Courier New" SIZE=2>______________________*
</FONT></BODY> </HTML>

Dr. Ahmed Hassaneen April 8, 2000 04:33

Re: Variable Density - Free Surface with FIDAP
 
Are you using the mixed, discontinous in the PRESSURE command or anything else? you should use it instead of the PENALTY method.

Costas Dimitropoulos April 8, 2000 16:46

Re: Variable Density - Free Surface with FIDAP
 
Hello:

Free surface problems are always tricky, especially when setting up the driving force of the surface deformation. We can't establish this a defect from the above information and we will take a look at this through our regular support channels and help the user accomplish his modeling objective. A brief resolution will be posted here once the support process is complete.

Let me stress that the best place to track supsected new defects that are obviously not yet confirmed or documented in the forum at Fluent's webiste is through your support engineer.

Vitaliy Pavlyk April 9, 2000 09:43

Re: Variable Density - Free Surface with FIDAP
 
Yes, the pressure is MIXED=0.1E-8 and DISCONTINUOUS.

A far as I know, the PENALTY can not be used because of : 1) the segregated solver invokes MIXED automatically; 2) a free surface analysis is not recommended with PENALTY; 3) compressible flow analysis (which can be solved by FIDAP only with the segregated solver ) is also not possible with PENALTY.

Vitaliy Pavlyk April 9, 2000 10:24

Re: Variable Density - Free Surface with FIDAP
 
Hi Costas,

thank you for attention and responce. I will take into account your comment. Indeed, my personal assumption about defect is not yet a subject for discussion here.

Best regards, =Vitaliy=


Ahmed Hassaneen April 11, 2000 05:32

Re: Variable Density - Free Surface with FIDAP
 
Hi Vitaliy, Would you please let me know the sequence you run the problem i.e. is it one run or two?? if you can send a copy from your FIPREP file that will be better. As a matter of fact my work is in the free jet impingement including free surface using FIDAP. There are so many things to be done here: 1- The gravity, body forces and surface tention value

2- The time step

3- The relaxation factors and the numbers of kinematic updates

4- You meight need to use CONTINUOUS instead of DISC

5- You meight need to solve the problem as a FIXED problem first and then use the READ RESTART to solve the FREE surface problem reading the temperatures from the previous run. These are some thoughts I'm not sure if it meight help but I have gone through all of them to solve my problem. Finally make sure that you are getting a converged solution with the segregated solver which meight take several hundreds of iterations. =Ahmed=

Vitaliy Pavlyk April 11, 2000 08:37

Re: Variable Density - Free Surface with FIDAP
 
Hi Ahmed,

Since the problem is transient, it is solved in a one run. Well, I solved it as FIXED and found , that the mass balance (the amount of fluid passed across the top of the glass) is satisfied. After the flow has reached steady-state, the temperature does not change any more (a constant temperature gradient was established, that's all), and the velocity is zero everywhere: no more expansion -> no more driving force for the momentum. You see, it has no sense to use such solution for RESTART with FREE surface.

The time step is small-fixed at the beginning and variable (truncation error = 1.0E-4) later on , and is mainly related to the energy equation.

The relaxation factors seems to be OK, since convergence is rather fast.

The kinematic updates (ONLY kinematic are used in a transient analysis) are = 50. But the SURFACE converges already with a few (normally 1) updates. Really, nothing is moving (to remember: only if FREE is specified), so the surface tolerance is about 1.0E-8 !!! after the first update.

CONTINUOUS ?? My previous experience tell me : better DISC. When the CONT was set in the problem under consideration, no influence on the surface behaviour was found. Instead, spurious velocities and pressure near the wall to be heated were observed.

You will find more details in the input files, that I sent to you. The test case is based on the example ex26sg.FDREAD from the FIDAP Example Manual.

I can describe it here too, if some body else has an interest.

Regards, - Vitaliy-


Costas Dimitropoulos May 2, 2000 15:56

Re: Variable Density - Free Surface with FIDAP
 
We have reviewed Vitaliy's problem. This is not really a bug. It is related to the fact that FIDAP can't support the mass constraint for confined compressible flows and is written for unconfined flows (such as flow in a pipe). This feauture is not difficult to implement and Vitaliy's question has reinforced the belief that we should provide this enhancement to FIDAP in the near future.

Sincerely,

COstas Dimitropoulos


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