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-   -   DFBI vs DEM (https://www.cfd-online.com/Forums/star-ccm/232151-dfbi-vs-dem.html)

SiemenDiemon December 1, 2020 17:51

DFBI vs DEM
 
Hi everyone,

I'm trying to decide on a method for modelling particles in fluid flow in STAR-CCM+. I'm new to this but having read through the documentation it seems the choice is between DEM (discrete element method) or DFBI (dynamic fluid-body interaction). I am being advised that DFBI is the more accurate of the two (and hence also more computationally intensive) but am curious what everyone else thinks. I'm guessing there would be cases where one is preferable over the other. For example the particle is morphable which makes me err towards DFBI.

As an aside, it also seems like DEM makes uses of some fairly complicated empirically derived formulae for calculating forces on a particle (e.g. lift coefficients) whereas DFBI seems to not do this. Am I understanding correctly that DFBI then just calculates the forces on a particle via the stress tensor?

Cheers!

ping December 3, 2020 03:20

dbfi is not really meant for use as a method to create and model particles since you would generally only have one or free bodies, but i have seen it done with maybe a dozen balls bouncing off each other - painful to setup unless a macro is used. the flow around the bodies is captured much better assume your overset meshes are good. but the contact physics in dbfi is very basic compared to dem.
dem is designed to model many particles together with complex interactions including contact, breakup, thermal, chemistry etc but as the particle numbers get up to 1e6 it gets very slow unless you have a big cluster.

SiemenDiemon January 24, 2021 18:14

Thanks Ping.

Yep, that seems to be the case. It's a shame that DEM is more suited for modelling particles as I'm struggling to find a way in the DEM framework to integrate the stress tensor over the surface of each particle to find the force more exactly, rather than using the built-in DEM force models which make some assumptions about the geometry of the particles.


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