Difference between revisions of "The DYCO Solver"

(Main features)
(Sample Results)
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We show below a short gallery of pictures obtained using the DYCO solver, in the context of   
 
We show below a short gallery of pictures obtained using the DYCO solver, in the context of   
 
{| class="wikitable"
 
{| class="wikitable"
|+ Sample results for 3D planar fronts  
+
|+ A sample 3D result including a non-homogeneous thermo-electric material with non-constant TE coefficients. 
|[[File:OUIImages_Luk.png|700 px]]
+
|[[File:OUITemperature.png|400 px]]
|}
+
|[[File:OUIPotential.png|400 px]]
{| class="wikitable"
+
|[[File:OUIElectricCurrent.png|400 px]]
|+ Sample results for 3D expanding fronts with variable turbulence intensity, 
+
|[[File:TroisFlammes.png|700 px]]
+
 
|}
 
|}
 +
BC are Homogeneous Neumann and Non-Homogeneous Dirichlet. Each elementary cell is of the non-ideal (non-linear) type.
  
 
==Sub-modules for ==
 
==Sub-modules for ==

Revision as of 11:57, 1 April 2016

The DYCO Solvers suite

Dyco96 Solvers.jpg

DYCO is a suite of solvers able to compute high accuracy solutions to non-linear

Main features

  • Solving

Sample Results

We show below a short gallery of pictures obtained using the DYCO solver, in the context of

A sample 3D result including a non-homogeneous thermo-electric material with non-constant TE coefficients.
OUITemperature.png OUIPotential.png OUIElectricCurrent.png

BC are Homogeneous Neumann and Non-Homogeneous Dirichlet. Each elementary cell is of the non-ideal (non-linear) type.

Sub-modules for

A sub-module of DYCO has been devoted to the numerical solution

System of equations, EEM and sample results of FB radius dynamics
Fbdynamics.png

Participants

Yves D'Angelo, Christophe Goupil, Eric Herbert, Xanthippi Zianni, Louise Meteir, Aurélie Louis-Napoléon.