Energy scaling law for the regular cone

TL;DR

This paper derives the energy scaling law for a thin elastic sheet shaped as a regular cone, showing it scales as $C^*h^2| ext{log} h|$ as thickness tends to zero, with an explicit constant.

Contribution

It introduces a fully nonlinear elastic energy model for a conical sheet and determines its precise energy scaling law as thickness diminishes.

Findings

Elastic energy scales as $C^*h^2| ext{log} h|$ for small thickness $h$

Explicit formula for the constant $C^*$ in the energy scaling law

Assumptions simplify the analysis by using exponential map and $L^ ext{infty}$ penalty

Abstract

We consider a thin elastic sheet in the shape of a disk whose reference metric is that of a singular cone. I.e., the reference metric is flat away from the center and has a defect there. We define a geometrically fully nonlinear free elastic energy, and investigate the scaling behavior of this energy as the thickness $h$ tends to 0. We work with two simplifying assumptions: Firstly, we think of the deformed sheet as an immersed 2-dimensional Riemannian manifold in Euclidean 3-space and assume that the exponential map at the origin (the center of the sheet) supplies a coordinate chart for the whole manifold. Secondly, the energy functional penalizes the difference between the induced metric and the reference metric in $L^\infty$ (instead of, as is usual, in $L^2$). Under these assumptions, we show that the elastic energy per unit thickness of the regular cone in the leading order of $h$ is given by $C^*h^2|\log h|$, where the value of $C^*$ is given explicitly.