CFD Simulations AC3-12: Difference between revisions

From KBwiki
Jump to navigation Jump to search
No edit summary
Line 7: Line 7:
'''Application Challenge AC3-12'''   © copyright ERCOFTAC 2013
'''Application Challenge AC3-12'''   © copyright ERCOFTAC 2013
==Overview of CFD Simulations==
==Overview of CFD Simulations==
Detailed numerical calculations were also performed  by  Sommerfeld  et al. (1992)
and Sommerfeld and  Qiu  (1993)  using  the  two-dimensional
axially-symmetric Euler/Lagrange approach without two-way coupling. The
fluid flow calculation is  based  on  the  time-averaged  Navier-Stokes
equations in connection with a closure assumption  for  the  turbulence
modelling. The solution of the above equations is obtained by using the
so-called FASTEST-code (Dimirdzic and Peric, 1990)  which  incorporates
the well-known k-ε two-equation turbulence model  and  uses  a  finite-
volume approach to descretize the equations. In order to  minimize  the
effects  of  numerical  diffusion  in  the  present  calculations,  the
quadratic, upwind-weighted differencing scheme  (QUICK)  was  used  for
differencing  the  convection  terms.  Furthermore,  flux-blending
techniques, where the convective flux can be calculated as  a  weighted
sum of the flux expressions from the "upwind"  and  QUICK  differencing
schemes (Peric et al., 1988),  was  used  to  avoid  instabilities  and
convergence problems that sometimes  appear  when  using  higher  order
schemes. The choice of the solution procedure described above was based
on  the  recommendations  of  Durst  and  Wennerberg  (1991)  who  also
concluded that for moderate swirl intensities the k-( turbulence  model
performs reasonably well.


==Computational Domain and Boundary Conditions Fluid Flow==
==Computational Domain and Boundary Conditions Fluid Flow==

Revision as of 09:56, 12 February 2013

Front Page

Description

Test Data

CFD Simulations

Evaluation

Best Practice Advice

Particle-laden swirling flow

Application Challenge AC3-12   © copyright ERCOFTAC 2013

Overview of CFD Simulations

Detailed numerical calculations were also performed by Sommerfeld et al. (1992) and Sommerfeld and Qiu (1993) using the two-dimensional axially-symmetric Euler/Lagrange approach without two-way coupling. The fluid flow calculation is based on the time-averaged Navier-Stokes equations in connection with a closure assumption for the turbulence modelling. The solution of the above equations is obtained by using the so-called FASTEST-code (Dimirdzic and Peric, 1990) which incorporates the well-known k-ε two-equation turbulence model and uses a finite- volume approach to descretize the equations. In order to minimize the effects of numerical diffusion in the present calculations, the quadratic, upwind-weighted differencing scheme (QUICK) was used for differencing the convection terms. Furthermore, flux-blending techniques, where the convective flux can be calculated as a weighted sum of the flux expressions from the "upwind" and QUICK differencing schemes (Peric et al., 1988), was used to avoid instabilities and convergence problems that sometimes appear when using higher order schemes. The choice of the solution procedure described above was based on the recommendations of Durst and Wennerberg (1991) who also concluded that for moderate swirl intensities the k-( turbulence model performs reasonably well.

Computational Domain and Boundary Conditions Fluid Flow

Modelling of Particle Phase




Contributed by: Martin Sommerfeld — Martin-Luther-Universitat Halle-Wittenberg

Front Page

Description

Test Data

CFD Simulations

Evaluation

Best Practice Advice


© copyright ERCOFTAC 2013