Presentation is loading. Please wait.

Presentation is loading. Please wait.

A hierarchy of theories for thin elastic bodies Stefan Müller MPI for Mathematics in the Sciences, Leipzig www.mis.mpg.de Bath Institute for Complex Systems.

Similar presentations


Presentation on theme: "A hierarchy of theories for thin elastic bodies Stefan Müller MPI for Mathematics in the Sciences, Leipzig www.mis.mpg.de Bath Institute for Complex Systems."— Presentation transcript:

1 A hierarchy of theories for thin elastic bodies Stefan Müller MPI for Mathematics in the Sciences, Leipzig www.mis.mpg.de Bath Institute for Complex Systems Multi-scale problems: Modelling, analysis and applications 12th – 14th September 2005

2 Nonlinear elasticity 3d  2d Major question since the beginning of elasticity theory Why ? 2d simpler to understand, visualize Important in engineering and biology Qualitatively new behaviour: crumpling, collapse Subtle influence of geometry (large rotations) Very non-scalar behaviour `Zoo of theories´ First rigorous results: LeDret-Raoult (´93-´96) (membrane theory,  -convergence) Acerbi-Buttazzo-Percivale (´91) (rods,  -convergence) Mielke (´88) (rods, centre manifolds)

3 Beyond membranes Key point: Low energy  close to rotation Classical result Need quantitative version

4 Rigidity estimate/ Nonlinear Korn Thm. (Friesecke, James, M.) Remarks 1. F. John (1961) u BiLip, dist (  u, SO(n)) <   Birth of BMO 2. Y.G. Reshetnyak Almost conformal maps: weak implies strong 3. Linearization  Korn´s inequality 4. Scaling is optimal (and this is crucial) 5. Ok for L p, 1 < p <  L 2 distance from a pointL 2 distance from a set

5 Rigidity estimate – an application Thm. (DalMaso-Negri-Percivale) 3d nonlinear elasticity 3d geom. linear elasticity L 2 distance from a pointL 2 distance from a set Gives rigorous status to singular solutions in linear elasticity Question: For which sets besides SO(n) does such an estimate hold ? Faraco-Zhong (quasiconformal), Chaudhuri-M. (2 wells), DeLellis-Szekelyhidi (abstract version)

6 Idea of proof 1. Four-line proof for (Reshetnyak, Kinderlehrer) 2. First part of the real proof: perturb this argument This yields (interior) bound by, not

7 Proof of rigidity estimate I Step 0: Wlog `truncation of gradients´ (Liu, Ziemer, Evans-Gariepy) Step1: Let Compute Take divergence

8 Proof of rigidity estimate II Step 2: We know Linearize at F = Id Set Korn  interior estimate with optimal scaling Step 3: Estimate up to the boundary. a)Cover by cubes with boundary distance  size b)Weighted Poincaré inequality (`Hardy ineq.´)

9 3d nonlinear elasticity

10 3d  2d Rem. Same for shells (FJM + M.G. Mora)

11 Gamma-convergence (De Giorgi)

12 The limit functional (Kirchhoff 1850) Geometrically nonlinear, Stress-strain relation linear (only matters) isometry „bending energy“ curvature

13 Idea of proof One key point: compactness 1.Unscale to S x (0,h), divide into cubes of size h 2.Apply rigidity estimate to each cube:  good approximation of deformation gradient by rotation 3.Apply rigidity estimate to union of two neighbouring cubes:  difference quotient estimate  compactness, higher differentiability of the limit

14 Different scaling limits (Modulo rigid motions) in-plane displacement out-of plane displacement Given  such that find , ,  for which

15 A hierarchy of theories (natural boundary conditions) For  > 2 assume that force points in a single direction (which can be assumed normal to the plate) and has zero moment

16 A hierarchy of theories (clamped boundary conditions, normal load)

17 Unified limit for  > 2 (natural bc)

18 Constrained theory for 2 <  < 4 One crucial ingredient for upper bound: Rem. Hartmann-Nirenberg, Pogorelov, Vodopyanov-Goldstein

19 A wide field The range is a no man‘s land where interesting things happen Two signposts:  = 1: Complex blistering patterns in thin films with Dirichlet boundary conditions Scaling known/ Gamma-limit open (depends on bdry cond. ?) BenBelgacem-Conti-DeSimone-M., Jin-Sternberg, Hornung  = 5/3: Crumpling of paper ? T. Witten et al., Pomeau, Ben Amar, Audoly, Mahadevan et al., Sharon et al., Venkataramani, Conti-Maggi,... More general: reduced theories which capture systematically both membrane and bending effects

20 Beyond minimizers (2d  1d)

21 A. Mielke, Centre manifolds

22 Conclusions Rigidity estimate/ Nonlinear Korn inequality Small energy  Close to rigid motion Beyond minimizers … Reduction 3d to 2d: Key point is geometry/ understanding (large) rotations (F. John)  Hierarchy of limiting theories ordered by scaling of the energy Interesting and largely unexplored scaling regimes where different limiting theories interact


Download ppt "A hierarchy of theories for thin elastic bodies Stefan Müller MPI for Mathematics in the Sciences, Leipzig www.mis.mpg.de Bath Institute for Complex Systems."

Similar presentations


Ads by Google