Dimension reduction for thin films with transversally varying prestrain: the oscillatory and the non-oscillatory case

Abstract

We study the non-Euclidean (incompatible) elastic energy functionals in the description of prestressed thin films, at their singular limits ($\Gamma$-limits) as $h\to 0$ in the film's thickness $h$. Firstly, we extend the prior results [Lewicka-Pakzad, Bhattacharya-Lewicka-Schaffner, Lewicka-Raoult-Ricciotti] to arbitrary incompatibility metrics that depend on both the midplate and the transversal variables (the "non-oscillatory" case). Secondly, we analyze a more general class of incompatibilities, where the transversal dependence of the lower order terms is not necessarily linear (the "oscillatory" case), extending the results of [Agostiniani-Lucic-Lucantonio, Schmidt] to arbitrary metrics and higher order scalings. We exhibit connections between the two cases via projections of appropriate curvature forms on the polynomial tensor spaces. We also show the effective energy quantisation in terms of scalings as a power of $h$ and discuss the scaling regimes $h^2$ (Kirchhoff), $h^4$ (von Kármán) in the general case, as well as all possible (even powers) regimes for conformal metrics, thus paving the way to the subsequent complete analysis of the non-oscillatory setting in [Lewicka]. Thirdly, we prove the coercivity inequalities for the singular limits at $h^2$- and $h^4$- scaling orders, while disproving the full coercivity of the classical von Kármán energy functional at scaling $h^4$.

arXiv commentAccepted in CPAM 2019

References in corpus (8)

• Elastic theory of unconstrained non-Euclidean plates
• Morphogenesis of growing soft tissues
• Programmed buckling by controlled lateral swelling in a thin elastic sheet
• A Riemannian Approach to Reduced Plate, Shell, and Rod Theories
• Shape selection in non-Euclidean plates
• Variational models for prestrained plates with Monge-Ampère constraint
• On the role of curvature in the elastic energy of non-Euclidean thin bodies
• The Monge-Ampere constrained elastic theories of shallow shells