TY - JOUR
T1 - On the spectrum of the finite element approximation of a three field formulation for linear elasticity
AU - Alzaben, Linda
AU - Bertrand, Fleurianne
AU - Boffi, Daniele
N1 - KAUST Repository Item: Exported on 2022-07-05
Acknowledgements: Fleurianne Bertrand gratefully acknowledges support by the German Research Foundation (DFG) in the Priority Programme SPP 1748 Reliable simulation techniques in solid mechanics under grant number BE6511/1-1. Daniele Boffi is member of the INdAM Research group GNCS and his research is partially supported by IMATI/CNR, Italy and by PRIN/MIUR, Italy .
PY - 2022/5/19
Y1 - 2022/5/19
N2 - We continue the investigation on the spectrum of operators arising from the discretization of partial differential equations. In this paper we consider a three field formulation recently introduced for the finite element least-squares approximation of linear elasticity. We discuss in particular the distribution of the discrete eigenvalues in the complex plane and how they approximate the positive real eigenvalues of the continuous problem. The dependence of the spectrum on the Lamé parameters is considered as well and its behavior when approaching the incompressible limit.
AB - We continue the investigation on the spectrum of operators arising from the discretization of partial differential equations. In this paper we consider a three field formulation recently introduced for the finite element least-squares approximation of linear elasticity. We discuss in particular the distribution of the discrete eigenvalues in the complex plane and how they approximate the positive real eigenvalues of the continuous problem. The dependence of the spectrum on the Lamé parameters is considered as well and its behavior when approaching the incompressible limit.
UR - http://hdl.handle.net/10754/670855
UR - https://linkinghub.elsevier.com/retrieve/pii/S2666657X22000155
U2 - 10.1016/j.exco.2022.100076
DO - 10.1016/j.exco.2022.100076
M3 - Article
SN - 2666-657X
VL - 2
SP - 100076
JO - Examples and Counterexamples
JF - Examples and Counterexamples
ER -