On the structure of layers for singularly perturbed equations in the case of unbounded energy
ESAIM: Control, Optimisation and Calculus of Variations (2010)
- 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 (2010): 941-963. <http://eudml.org/doc/90680>.
@article{Sanchez2010,
abstract = {
We consider singular perturbation variational problems
depending on a small parameter ε. The right hand side is such
that the energy
does not remain bounded as ε → 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 ε > 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.; propagation of singularities; distribution right hand sides},
language = {eng},
month = {3},
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/90680},
volume = {8},
year = {2010},
}
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
DA - 2010/3//
PB - EDP Sciences
VL - 8
SP - 941
EP - 963
AB -
We consider singular perturbation variational problems
depending on a small parameter ε. The right hand side is such
that the energy
does not remain bounded as ε → 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 ε > 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.; propagation of singularities; distribution right hand sides
UR - http://eudml.org/doc/90680
ER -
References
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- M.I. Vishik and L. Lusternik, Regular degenerescence and boundary layer for linear differential equations with small parameter.Usp. Mat. Nauk12 (1957) 1-122.
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