Difference between revisions of "SiTCom-B Gallery"

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(Immersed boundaries in LES of compressible flows)
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* G. Lodier, C. Merlin, P. Domingo, L. Vervisch, F. Ravet (2012) Self-ignition scenarios after rapid compression of a turbulent mixture weakly-stratified in temperature, Combust. Flame 159(11): 3358-3371.
 
* G. Lodier, C. Merlin, P. Domingo, L. Vervisch, F. Ravet (2012) Self-ignition scenarios after rapid compression of a turbulent mixture weakly-stratified in temperature, Combust. Flame 159(11): 3358-3371.
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== Mixing time-history effects: Flow-Controlled Chemistry Tabulation ==
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{| class="wikitable"
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|+ Analysis of time-history of turbulent mixing and fully new approach to turbulent combustion modeling
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|-
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| [[File:FCCT1.png|center|400px]]
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| [[File:FCCT2.png|center|400px]]
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| [[File:FCCT3.png|center|400px]]
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|-
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| FCCT procedure
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| Dynamic construction of advanced chemistry tabulation
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| Turbulent flame response to micro-mixing history
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|}
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* N. Enjalbert, P. Domingo, L. Vervisch, F. Ravet (2012) Mixing time-history effects in Large Eddy Simulation of non-premixed turbulent flames: Flow-Controlled Chemistry Tabulation, Combust. Flame 159(1): 336-352.
  
 
== DNS of a non-reacting HIT ==
 
== DNS of a non-reacting HIT ==

Revision as of 11:28, 6 November 2012

LES of a Trapped Vortex Combustor

Immersed boundaries are used to optimize the geometry of a trapped vortex combustor
TVC1.png
TVC2.png
 
TVC3.png
Geometry of the Trapped Vortex Combustion chamber Q-critrion - Visualisation of the turbulent flow topology Comparison against experiments
  • C. Merlin, P. Domingo, L. Vervisch Large Eddy Simulation of turbulent flames in a Trapped Vortex Combustor (TVC) - A flamelet presumed-pdf closure preserving laminar flame speed, Comptes Rendus Mecanique, Out of Equilibrium Dynamics issue, in press.

Immersed boundaries in LES of compressible flows

Immersed boundaries are developed for fully compressible simulations
IBM1.png
IBM2.png
 
IBM3.png
Pressure wave reflection on inclined walls Transonic cavity flow simulation Comparison of pressure spectra against measurements
  • C. Merlin, P. Domingo, L. Vervisch Immersed Boundaries in Large Eddy Simulation of Compressible Flows, Flow Turbulence and Combustion, DOI 10.1007/s10494-012-9421-0

DNS of a Rapid Compression Machine

Analysis of ignition regimes after rapid compression - Homogeneous mixture stratified in temperature
RCM1.png
RCM2.png
 
RCM3.png
Flow injection sequence - Resolution of Ignition patterns Regime Diagram
  • G. Lodier, C. Merlin, P. Domingo, L. Vervisch, F. Ravet (2012) Self-ignition scenarios after rapid compression of a turbulent mixture weakly-stratified in temperature, Combust. Flame 159(11): 3358-3371.

Mixing time-history effects: Flow-Controlled Chemistry Tabulation

Analysis of time-history of turbulent mixing and fully new approach to turbulent combustion modeling
FCCT1.png
FCCT2.png
 
FCCT3.png
FCCT procedure Dynamic construction of advanced chemistry tabulation Turbulent flame response to micro-mixing history
  • N. Enjalbert, P. Domingo, L. Vervisch, F. Ravet (2012) Mixing time-history effects in Large Eddy Simulation of non-premixed turbulent flames: Flow-Controlled Chemistry Tabulation, Combust. Flame 159(1): 336-352.

DNS of a non-reacting HIT

This is a very simple DNS computation of a HIT with a constant-properties gas.
The main parameters of the simulation are:

  • temporal integration: RK3,
  • spatial scheme: 4th order skew symmetric
  • no AV.

In this series of computations, the number of cell is increased from 64^3 to 256^3.

HIT on increasing number of cells. The displayed field is
HIT 0064cube.png
HIT 0128cube.png
HIT 0256cube.png


DNS of a non-reacting supercritical mixing layer

This simulation is a DNS of a HIT non-reacting supercritical mixing layer with real-gas properties (equation of state, thermodynamic laws and transport laws).
The main parameters of the simulation are:

  • temporal integration: RK3,
  • spatial scheme: 4th order skew symmetric
  • 2D / Periodic in all directions
  • 3.2 Million cells
  • EOS: Soave-Redlich-Kwong.
  • Transport laws: Chung et al.

Supercritical Mixing Layer

The fields that are displayed are:

  • up : the density which varies from 80 kg/m3 in the cold stream to 800 kg/m3 in the hot stream.
  • down : the mixness ratio which varies from 0 in pure constitutents to 1 for perfect mixness.




Media:supercritical_mixing_layer_mix.avi


This video shows the temporal evolution of mixness ratio during the simulation.
Warning:

  • no Artificial Viscosity was used and the mesh was slightly too coarse: a few "wiggles" are visible from time to time near the steepest gradients...
  • this video is best visualized with VLC.


Flame base stabilization in vitiated partially-premixed mixture

Nice QW.png

  • P. Domingo, L. Vervisch, D. Veynante (2008) Large-Eddy Simulation of a lifted methane jet flame in a vitiated coflow Combust. Flame 152(3): 415-432.


Electric field and edge-flame

Electric edges 1.png

  • M. Belhi, P. Domingo, P. Vervisch (2010) Direct numerical simulation of the effect of an electric field on flame stability Combust. Flame 157 2286–2297.


NSCBC vs 3D-NSCBC in jets

Jet NSCBC 1D.png Jet 3DNSCBC bis.png

  • G. Lodato, P. Domingo, L. Vervisch (2008) Three-dimensional boundary conditions for Direct and Large-Eddy Simulation of compressible flows J. of Comp. Phys. 227(10): 5105-5143.


Impinging round jets

Wall/jet interaction Jet wall 1.png]]

Jet wall 2.png Jet wall 3.png

  • G. Lodato, L. Vervisch, P. Domingo (2009) A compressible wall-adapting similarity mixed model for large-eddy simulation of the impinging round jet Phys. Fluids 21:035102.


Ignition of a bluff-body burner

Igni bluff 1.png

  • V. Subramanian, P. Domingo, L. Vervisch (2010) Large-Eddy Simulation of forced ignition of an annular bluff-body burner Combust. Flame 157(3): 579-601.


Bunsen flame

Bunsen.png

  • G. Lodato, P. Domingo, L. Vervisch, D. Veynante (2009) Scalar variances: LES against measurements and mesh optimization criterion; scalar gradient: a three-dimensional estimation from planar measurements using DNS In Studying turbulence by using numerical simulation databases XII, (Eds Center for Turbulence Research) Stanford, pp. 387-398


Jet flame-surface

Jet flame DNS.png

  • L. Vervisch, P. Domingo, G. Lodato, D. Veynante (2010) Scalar energy fluctuations in Large-Eddy Simulation of turbulent flames: Statistical budgets and mesh quality criterion Combust. Flame 157(4): 778-789.
  • D. Veynante, G. Lodato, P. Domingo, L. Vervisch, E. R. Hawkes (2010) Estimation of three-dimensional flame surface densities from planar images in turbulent premixed combustion Exp. in Fluids 49:267-278.


Nonpremixed jet flame

Sandia flame.png

  • G. Godel, P. Domingo, L. Vervisch (2009) Tabulation of NOx chemistry for Large-Eddy Simulation of non-premixed turbulent flames Proc. Combust. Inst. 32: 1555-1551.