|October 4, 2001, 05:57||
Can anyone tell me how to go about modifying the non-Newtonian Power-Law viscosity in Fluent to include a true yield stress, which would make it a Herschel Bulkley viscosity? I know this would be via a UDF, but is there any way I can get access to the existing code for Power-Law viscosity and then modify it as a UDF? Or do I have to start a UDF from scratch myself, and if so, how? Thanks in advance
|October 4, 2001, 10:06||
Re: Hershel-Bulkley viscosity
I have been working for a long time in the area of viscoplastic fluids and have already experienced to include this kind of models (Bingham or Helschel-Bulkley) in Fluent. Concerning that point, I have two news for you : a good one and a bad one
1. good new : implementing visoplastic fluids in Fluent works very well !! and besides is very easy to handle. You only have to write an UDF for the viscosity.
2. bad new : for confidentiality reasons (I am currently working for a private company), I cannot forward you the UDF.
Nevertheless, I encourage you to try too because you are now absolutely sure that it will work (if you trust me of course). And I can show you how to consider the model in Fluent because obviously, after a deep look in the literature, you would probably find it by yourself, so I expect that the following tips will enable you to save some time.
Consider the Bingham constitutive equation in 3D (the generalization to HB model is straightforward) :
gamma=(second invariant of D)=sqrt(2*tr(D**2))
If you write this relation in terms of apparent viscosity mu_a, it yields :
An other thing to keep in mind is that the relation tau=f(D) or tau=f(gamma) in 1D (in that case, gamma is the shear rate) is discontinuous in gamma=0 and tau cannot be evaluated (for gamma=0, tau in [0,tau_0]). A popular solution consists in using any of the following regularization models :
1. bi-viscosity model
2. exponential model
3. model with a parameter epsilon
I chose to use the exponential model which can be written as :
with m=numerical parameter
If m is great enough (typical values verify m>100), the regularized law fits well the real consitutive equation. Thus, your regularized law exhibit now good properties : continuous (stress can be computed everywhere e.g. tau in [0,infinity]) and is differentiable everywhere too e.g. is C^infinity.
This method to tackle viscoplastic problems is well known and works very well with Fluent too either in 1D or in 2D-3D problems.
Have a look to those papers : 1. T.C. Papnastasiou "Flow of materials with yield", Journal of Rheology, 31, 385-404, (1987).
2. E. Mitsoulis, S.S. Abdali, N.C. Markatos, "Flow simulation of Herschel-Bulkley fluids through extrusion dies, Canadian Journal of Chemical Engineering, 71, 147-160, 1993.
3. M. Beaulne, E. Mitsoulis, "Creeping motion of a sphere in tubes filled with Herschel-Bulkley fluids", Journal of Non Newtonian Fluid Mechanics, 72, 55-71, 1997.
4. J. Blackery, E. Mitsoulis, "Creeping motion of a sphere in tubes filled with a Bingham plastic material", Journal of Non Newtonian Fluid Mechanics, 70, 59-77, (1997).
5. I.C. Walton, S.H. Bittleston, "The axial flow of a Bongham plastic in a narrow eccentric annulus", Journal of Fluid Mechanics", 222, 39-60, (1991).
With all those informations, I am quite sure you will succeed !! The only remaining thing to do by yourself is to write the UDF for the apparent viscosity (forget about the non-newtonian power law that is not suited to handle yield stress), that is an easy and quick duty.
Hope it might help you...
|April 3, 2013, 11:51||
Join Date: Apr 2013
Posts: 1Rep Power: 0
hi, Do you know whether liquefied iron ore powder is the viscoplastic fluid\?
I think I should do some steps:
1: do some experiments about the material
2: build the constitutive equation using the UDF
|February 4, 2014, 02:41||
Join Date: Jun 2012
Posts: 30Rep Power: 5
I am also trying to solve a similar problem. where should I attach the udf in fluent because if I attach it to viscosity, I don't find any place to enter the value of power n and consistency index K
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