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== ''Participants'' == | == ''Participants'' == | ||
[http://www.dyco.fr/index.php/User:Yd Yves D'Angelo], [http://www.dyco.fr/index.php/User:Cg Christophe Goupil], [http://www.dyco.fr/index.php/User:Eh Eric Herbert], [http://xzianni.aero.teiste.gr/ Xanthippi Zianni], [http://www.dyco.fr/index.php/Lm Louise Méteier], [http://www.dyco.fr/index.php/Aln Aurélie Louis-Napoléon]. | [http://www.dyco.fr/index.php/User:Yd Yves D'Angelo], [http://www.dyco.fr/index.php/User:Cg Christophe Goupil], [http://www.dyco.fr/index.php/User:Eh Eric Herbert], [http://xzianni.aero.teiste.gr/ Xanthippi Zianni], [http://www.dyco.fr/index.php/Lm Louise Méteier], [http://www.dyco.fr/index.php/Aln Aurélie Louis-Napoléon]. | ||
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Revision as of 10:54, 8 April 2016
DyCo also stands for Dynamiques Couplées ! (in French).
The DYCO Solvers suite
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.
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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 dependency can also be included.
- Local flux continuity enforced
- 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.
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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.
The numerical solution to the coupling between 1D/3D Maxwell and heat equations is also in progress.
Participants
Yves D'Angelo, Christophe Goupil, Eric Herbert, Xanthippi Zianni, Louise Méteier, Aurélie Louis-Napoléon.
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