Éléments finis mixtes incompressibles pour l'équation de Stokes dans ℝ3
JC Nédélec - Numerische Mathematik, 1982 - dl.acm.org
We introduce some new families of finite element approximation for the stationary Stokes
and Navier Stokes equations in a bounded domain in 3. These elements can used …
and Navier Stokes equations in a bounded domain in 3. These elements can used …
Integral equations with non integrable kernels
JC Nedelec - Integral equations and operator theory, 1982 - Springer
We study here some integral equations linked to the Laplace or the Helmholtz equation, or
to the system of elasticity equations. These equations lead to non integrable kernels only …
to the system of elasticity equations. These equations lead to non integrable kernels only …
Des préconditionneurs pour la résolution numérique des équations intégrales de frontière de l'acoustique
SH Christiansen, JC Nédélec - Comptes Rendus de l'Académie des …, 2000 - Elsevier
Nous étendons la méthode de préconditionnement introduite par O. Steinbach et WL
Wendland dans 7 aux opérateurs satisfaisant des conditions Inf-Sup. Nous associons ainsi à la …
Wendland dans 7 aux opérateurs satisfaisant des conditions Inf-Sup. Nous associons ainsi à la …
[PDF][PDF] Une méthode variationnelle d'éléments finis pour la résolution numérique d'un probleme extérieur dans
JC Nédélec, J Planchard - Revue française d'automatique informatique …, 1973 - numdam.org
… Réciproquement si la distribution q est donnée dans l'espace H~lf2(T) le problème
variationnel (1.14) admet une solution unique u dans JF<J(R3) d'après la propriété de l'expression …
variationnel (1.14) admet une solution unique u dans JF<J(R3) d'après la propriété de l'expression …
Time-harmonic electromagnetic fields in thin chiral curved layers
H Ammari, JC Nédélec - SIAM Journal on Mathematical Analysis, 1998 - SIAM
In this paper, we prove existence and uniqueness of the solution to the diffraction problem of
a plane electromagnetic field by a chiral curved layer covering a perfectly conducting object…
a plane electromagnetic field by a chiral curved layer covering a perfectly conducting object…
[HTML][HTML] Bioactive glass nanoparticles: from synthesis to materials design for biomedical applications
C Vichery, JM Nedelec - Materials, 2016 - mdpi.com
… Jean-Marie Nedelec would like to thank the Guest Editor of this Special Issue, Gigliola …
Charlotte Vichery and Jean-Marie Nedelec equally contributed to the writing and correction …
Charlotte Vichery and Jean-Marie Nedelec equally contributed to the writing and correction …
Biological properties of copper-doped biomaterials for orthopedic applications: A review of antibacterial, angiogenic and osteogenic aspects
A Jacobs, G Renaudin, C Forestier, JM Nedelec… - Acta biomaterialia, 2020 - Elsevier
Copper is an essential trace element required for human life, and is involved in several
physiological mechanisms. Today researchers have found and confirmed that Cu has biological …
physiological mechanisms. Today researchers have found and confirmed that Cu has biological …
[BOOK][B] Acoustic and electromagnetic equations: integral representations for harmonic problems
JC Nédélec - 2001 - Springer
This book is devoted to the study of the acoustic wave equation and of the Maxwell system,
the two most common wave equations encountered in physics or in engineering. The main …
the two most common wave equations encountered in physics or in engineering. The main …
Use of sacrificial anodes in electrochemical functionalization of organic halides
J Chaussard, JC Folest, JY Nedelec, J Perichon… - …, 1990 - thieme-connect.com
… Jacques Chaussard,“ Jean-Claude Folest,“ J ean-Yves Nedelec,‘J Jacques Perichon,b
Soline Sibille,b Michel Troupelb “ Centre de Recherches du Bouchet de la Société …
Soline Sibille,b Michel Troupelb “ Centre de Recherches du Bouchet de la Société …
A justification of eddy currents model for the Maxwell equations
… Due to (2.4) the current source J has to satisfy some compatibility conditions. In particular, …
function J is then the curl of the magnetic field H. In order to characterize this constraint on J, …
function J is then the curl of the magnetic field H. In order to characterize this constraint on J, …