Difference between revisions of "The DYCO Solver"

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It is based on a nodal approach strategy.  
 
It is based on a nodal approach strategy.  
 
{| class="wikitable"
 
{| class="wikitable"
|[[File:Imuz.png|450 px]]
+
|[[File:Imuz.png|350 px]]
|[[File:ImuzSerie.png|150 px]]
+
|[[File:ImuzSerie.png|120 px]]
|[[File:Sfte.png|350 px]]
+
|[[File:Sfte.png|250 px]]
 
|}
 
|}
 
Left: Elementary Cell, Coupled potentials (1 or N coupled potentials, also in series) <br/ >
 
Left: Elementary Cell, Coupled potentials (1 or N coupled potentials, also in series) <br/ >
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{| class="wikitable"
 
{| class="wikitable"
 
|+ Sample 3D results  including a non-homogeneous thermo-electric material with non-constant TE coefficients.   
 
|+ Sample 3D results  including a non-homogeneous thermo-electric material with non-constant TE coefficients.   
|[[File:OUITemperature.png|350 px]]
+
|[[File:OUITemperature.png|300 px]]
|[[File:OUIPotential.png|400 px]]
+
|[[File:OUIPotential.png|340 px]]
|[[File:OUIElectricCurrent.png|400 px]]
+
|[[File:OUIElectricCurrent.png|340 px]]
 
|}
 
|}
 
{| class="wikitable"
 
{| class="wikitable"
 
|+ Sample 3D results  for N-type junction with non-constant noisy TE coefficients.   
 
|+ Sample 3D results  for N-type junction with non-constant noisy TE coefficients.   
|[[File:OUIEnergyDensity3D.png|400 px]]
+
|[[File:OUIEnergyDensity3D.png|300 px]]
|[[File:OUIEntropyProduction.png|350 px]]
+
|[[File:OUIEntropyProduction.png|220 px]]
 
|}
 
|}
 
In both cases, BC are Homogeneous Neumann and/or Non-Homogeneous Dirichlet. <br/ >
 
In both cases, BC are Homogeneous Neumann and/or Non-Homogeneous Dirichlet. <br/ >

Revision as of 20:30, 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 stock/flow potentials coupled equations.
It is based on a nodal approach strategy.

Imuz.png ImuzSerie.png Sfte.png

Left: Elementary Cell, Coupled potentials (1 or N coupled potentials, also in series)
Right: example in the thermo-electric context

Main features

  • Nodal description of the considered network.
  • Non linear Onsager type coupling between forces & fluxes.
  • Steady, pseudo-unsteady & unsteady computations.
  • Handle local to global scales (i.e. from coarse-grain to fine tuning).
  • Possibly complex non-homogeneous structures and topologies.
  • Possibly anisotropic, discontinuous coupling coefficients; potentials & time dependence can also be included.
  • Allows for lighter/heavier computations and technological “optimization” !

Sample Results

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

Sample 3D results including a non-homogeneous thermo-electric material with non-constant TE coefficients.
OUITemperature.png OUIPotential.png OUIElectricCurrent.png
Sample 3D results for N-type junction with non-constant noisy TE coefficients.
OUIEnergyDensity3D.png OUIEntropyProduction.png

In both cases, BC are Homogeneous Neumann and/or Non-Homogeneous Dirichlet.
Each elementary cell is of the non-ideal (non-linear) type.

Sub-modules

More specific sub-modules of DYCO shall be devoted to the numerical solution of coupled stock/flow potentials
dynamics in the ecological economics and biological contexts.

Participants

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