(→The DYCO Team Members) |
(→The DYCO Team) |
||
| Line 25: | Line 25: | ||
|[[File:OUILeontiefTotal.jpg|430 px]] | |[[File:OUILeontiefTotal.jpg|430 px]] | ||
|} | |} | ||
| + | |||
| + | |||
| + | <!DOCTYPE html> | ||
| + | <html> | ||
| + | <head> | ||
| + | <title>MathJax TeX Test Page</title> | ||
| + | <script type="text/x-mathjax-config"> | ||
| + | MathJax.Hub.Config({tex2jax: {inlineMath: [['$','$'], ['\\(','\\)']]}}); | ||
| + | </script> | ||
| + | <script type="text/javascript" async | ||
| + | src="https://cdn.mathjax.org/mathjax/latest/MathJax.js?config=TeX-AMS_CHTML"> | ||
| + | </script> | ||
| + | </head> | ||
| + | <body> | ||
| + | When $a \ne 0$, there are two solutions to \(ax^2 + bx + c = 0\) and they are | ||
| + | $$x = {-b \pm \sqrt{b^2-4ac} \over 2a}.$$ | ||
| + | </body> | ||
| + | </html> | ||
Revision as of 11:13, 3 April 2016
The DYCO Team
Research
Our research activities mainly deal with the modeling, simulation & analysis of the dynamics of coupled potentials, in an Onsager-type force/flux approach.
Present applications are network thermodynamics, thermoelectricity, ecological economics, network stress signaling in plants, and also, in the context of fluid dynamics, the buoyant destabilization of wet granular or non-Newtonian media, and the thermo-electric Rayleigh-Bénard instability.
See our recent publications.
The DYCO Team Members
- Christophe Goupil, Full Professor of Physics - Paris Diderot University
- Eric Herbert, Associate Professor of Physics - Paris Diderot University
- Yves D'Angelo, Full Professor of Applied Mathematics & Fluid Dynamics - INSA Rouen
|
|
<!DOCTYPE html>
<html>
<head>
<title>MathJax TeX Test Page</title>
<script type="text/x-mathjax-config">
MathJax.Hub.Config({tex2jax: {inlineMath: [['$','$'], ['\\(','\\)']]}});
</script> <script type="text/javascript" async
src="https://cdn.mathjax.org/mathjax/latest/MathJax.js?config=TeX-AMS_CHTML">
</script> </head> <body> When $a \ne 0$, there are two solutions to \(ax^2 + bx + c = 0\) and they are $$x = {-b \pm \sqrt{b^2-4ac} \over 2a}.$$ </body> </html>