TY - JOUR
T1 - On the approximation of electromagnetic fields by edge finite elements—Part 4
T2 - analysis of the model with one sign-changing coefficient
AU - Ciarlet, Patrick
N1 - Publisher Copyright:
© 2022, The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature.
PY - 2022/10/1
Y1 - 2022/10/1
N2 - In electromagnetism, in the presence of a negative material surrounded by a classical material, the electric permittivity, and possibly the magnetic permeability, can exhibit a sign-change at the interface. In this setting, the study of electromagnetic phenomena is a challenging topic. We focus on the time-harmonic Maxwell equations in a bounded set Ω of R3, and more precisely on the numerical approximation of the electromagnetic fields by edge finite elements. Special attention is paid to low-regularity solutions, in terms of the Sobolev scale (Hs(Ω))s>0. With the help of T-coercivity, we address the case of one sign-changing coefficient, both for the model itself, and for its discrete version. Optimal a priori error estimates are derived.
AB - In electromagnetism, in the presence of a negative material surrounded by a classical material, the electric permittivity, and possibly the magnetic permeability, can exhibit a sign-change at the interface. In this setting, the study of electromagnetic phenomena is a challenging topic. We focus on the time-harmonic Maxwell equations in a bounded set Ω of R3, and more precisely on the numerical approximation of the electromagnetic fields by edge finite elements. Special attention is paid to low-regularity solutions, in terms of the Sobolev scale (Hs(Ω))s>0. With the help of T-coercivity, we address the case of one sign-changing coefficient, both for the model itself, and for its discrete version. Optimal a priori error estimates are derived.
U2 - 10.1007/s00211-022-01315-x
DO - 10.1007/s00211-022-01315-x
M3 - Article
AN - SCOPUS:85138203018
SN - 0029-599X
VL - 152
SP - 223
EP - 257
JO - Numerische Mathematik
JF - Numerische Mathematik
IS - 2
ER -