A Highly Anisotropic Nonlinear Elasticity Model for Vesicles II: Derivation of the Thin Bilayer Bending Theory

Verfasser / Beitragende:
[Benoît Merlet]
Ort, Verlag, Jahr:
2015
Enthalten in:
Archive for Rational Mechanics and Analysis, 217/2(2015-08-01), 681-740
Format:
Artikel (online)
ID: 605515638
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024 7 0 |a 10.1007/s00205-014-0840-z  |2 doi 
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100 1 |a Merlet  |D Benoît  |u Centre de Mathématiques Appliquées (CMAP), Ecole Polytechnique, 91128, Palaiseau, France  |4 aut 
245 1 2 |a A Highly Anisotropic Nonlinear Elasticity Model for Vesicles II: Derivation of the Thin Bilayer Bending Theory  |h [Elektronische Daten]  |c [Benoît Merlet] 
520 3 |a We study the thin-shell limit of the nonlinear elasticity model for vesicles introduced in part I. We consider vesicles of width $${2 \varepsilon \downarrow 0}$$ 2 ε ↓ 0 with elastic energy of order $${\varepsilon^3}$$ ε 3 . In this regime, we show that the limit model is a bending theory for generalized hypersurfaces—namely, co-dimension one oriented varifolds without boundary. Up to a positive factor, the limit functional is the Willmore energy. In the language of $${{\it \Gamma}}$$ Γ -convergence, we establish a compactness result, a lower bound result and the matching upper bound in the smooth case. 
540 |a Springer-Verlag Berlin Heidelberg, 2015 
773 0 |t Archive for Rational Mechanics and Analysis  |d Springer Berlin Heidelberg  |g 217/2(2015-08-01), 681-740  |x 0003-9527  |q 217:2<681  |1 2015  |2 217  |o 205 
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900 7 |a Metadata rights reserved  |b Springer special CC-BY-NC licence  |2 nationallicence 
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950 |B NATIONALLICENCE  |P 856  |E 40  |u https://doi.org/10.1007/s00205-014-0840-z  |q text/html  |z Onlinezugriff via DOI 
950 |B NATIONALLICENCE  |P 100  |E 1-  |a Merlet  |D Benoît  |u Centre de Mathématiques Appliquées (CMAP), Ecole Polytechnique, 91128, Palaiseau, France  |4 aut 
950 |B NATIONALLICENCE  |P 773  |E 0-  |t Archive for Rational Mechanics and Analysis  |d Springer Berlin Heidelberg  |g 217/2(2015-08-01), 681-740  |x 0003-9527  |q 217:2<681  |1 2015  |2 217  |o 205