Difference between revisions of "The DYCO Solver"

Revision as of 11:04, 1 April 2016

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

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.

Sample 3D results for N-type junction with non-constant noisy TE coefficients.

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

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

System of equations, EEM and sample results of FB radius dynamics

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

@@ Line 8: / Line 8: @@
 == Sample Results ==
-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 thermo-electric context.
 {| class="wikitable"
 |+ Sample 3D results  including a non-homogeneous thermo-electric material with non-constant TE coefficients.
@@ Line 15: / Line 15: @@
 |[[File:OUIElectricCurrent.png|400 px]]
 |}
-BC are Homogeneous Neumann and Non-Homogeneous Dirichlet. Each elementary cell is of the non-ideal (non-linear) type.
 {| class="wikitable"
@@ Line 23: / Line 21: @@
 |[[File:OUIEntropyProduction.png|350 px]]
 |}
+In both cases, BC are Homogeneous Neumann and/or Non-Homogeneous Dirichlet.
+Each elementary cell is of the non-ideal (non-linear) type.
-BC are Homogeneous Neumann and/or Non-Homogeneous Dirichlet. Each elementary cell is of the non-ideal (non-linear) type.
 ==Sub-modules for ==