On the structure of layers for singularly perturbed equations in the case of unbounded energy
ESAIM: Control, Optimisation and Calculus of Variations (2002)
- Volume: 8, page 941-963
- ISSN: 1292-8119
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topSanchez-Palencia, E.. "On the structure of layers for singularly perturbed equations in the case of unbounded energy." ESAIM: Control, Optimisation and Calculus of Variations 8 (2002): 941-963. <http://eudml.org/doc/245292>.
@article{Sanchez2002,
abstract = {We consider singular perturbation variational problems depending on a small parameter $ \varepsilon $. The right hand side is such that the energy does not remain bounded as $ \varepsilon \rightarrow 0 $. The asymptotic behavior involves internal layers where most of the energy concentrates. Three examples are addressed, with limits elliptic, parabolic and hyperbolic respectively, whereas the problems with $ \varepsilon >0 $ are elliptic. In the parabolic and hyperbolic cases, the propagation of singularities appear as an integral property after integrating across the layers.},
author = {Sanchez-Palencia, E.},
journal = {ESAIM: Control, Optimisation and Calculus of Variations},
keywords = {singular perturbations; unbounded energy; propagation of singularities; distribution right hand sides},
language = {eng},
pages = {941-963},
publisher = {EDP-Sciences},
title = {On the structure of layers for singularly perturbed equations in the case of unbounded energy},
url = {http://eudml.org/doc/245292},
volume = {8},
year = {2002},
}
TY - JOUR
AU - Sanchez-Palencia, E.
TI - On the structure of layers for singularly perturbed equations in the case of unbounded energy
JO - ESAIM: Control, Optimisation and Calculus of Variations
PY - 2002
PB - EDP-Sciences
VL - 8
SP - 941
EP - 963
AB - We consider singular perturbation variational problems depending on a small parameter $ \varepsilon $. The right hand side is such that the energy does not remain bounded as $ \varepsilon \rightarrow 0 $. The asymptotic behavior involves internal layers where most of the energy concentrates. Three examples are addressed, with limits elliptic, parabolic and hyperbolic respectively, whereas the problems with $ \varepsilon >0 $ are elliptic. In the parabolic and hyperbolic cases, the propagation of singularities appear as an integral property after integrating across the layers.
LA - eng
KW - singular perturbations; unbounded energy; propagation of singularities; distribution right hand sides
UR - http://eudml.org/doc/245292
ER -
References
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- [5] P. Karamian and J. Sanchez–Hubert, Boundary layers in thin elastic shells with developable middle surface. Eur. J. Mech., A/Solids 21 (2002) 13-47. Zbl1006.74064
- [6] P. Karamian, J. Sanchez–Hubert and E. Sanchez–Palencia, Propagation of singularities and structure of the layers in shells. Hyperbolic case. Comp. and Structures (to appear).
- [7] J.-L. Lions, Perturbations singulières dans les problèmes aux limites et en contrôle optimal. Springer, Berlin (1973). Zbl0268.49001MR600331
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- [9] J.-L. Lions and E. Sanchez–Palencia, Sensitivity of certain constrained systems and application to shell theory. J. Math. Pures Appl. 79 (2000) 821-838. Zbl1013.74050
- [10] E. Sanchez–Palencia, On a singular perturbation going out of the energy space. J. Math. Pures. Appl. 79 (2000) 591-602. Zbl0958.35008
- [11] E. Sanchez–Palencia, Singular perturbations going out of the energy space. Layers in elliptic and parabolic cases, in Proc. of the 4th european Conference on Elliptic and Parabolic Problems. Rolduc-Gaeta, edited by Bemelmans et al. World Scientific Press (2002). Zbl1033.35010
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