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Wrinkling of an elastic sheet floating on a liquid sphere

Peter Bella, Carlos Román

Abstract

A thin circular elastic sheet floating on a drop-like liquid substrate is deformed due to incompatibility between the curved substrate and the planar sheet. We adopt a variational viewpoint by minimizing the non-convex membrane energy together with a higher-order convex bending energy. Focusing on thin sheets, we expand the minimum of the energy in terms of a small thickness ratio $h$, and identify the first two terms of this expansion. The leading-order term arises from the minimization of a family of one-dimensional relaxed problems, while for the next-order term we establish lower and upper bounds. This generalizes the previous work [P. Bella and R.V. Kohn. Wrikling of a thin circular sheet bonded to a spherical substrate, Philos. Trans. Roy. Soc. A, 375(2017). arXiv:1611.01781] to the physically relevant case of a liquid substrate.

Wrinkling of an elastic sheet floating on a liquid sphere

Abstract

A thin circular elastic sheet floating on a drop-like liquid substrate is deformed due to incompatibility between the curved substrate and the planar sheet. We adopt a variational viewpoint by minimizing the non-convex membrane energy together with a higher-order convex bending energy. Focusing on thin sheets, we expand the minimum of the energy in terms of a small thickness ratio , and identify the first two terms of this expansion. The leading-order term arises from the minimization of a family of one-dimensional relaxed problems, while for the next-order term we establish lower and upper bounds. This generalizes the previous work [P. Bella and R.V. Kohn. Wrikling of a thin circular sheet bonded to a spherical substrate, Philos. Trans. Roy. Soc. A, 375(2017). arXiv:1611.01781] to the physically relevant case of a liquid substrate.
Paper Structure (17 sections, 5 theorems, 54 equations)

This paper contains 17 sections, 5 theorems, 54 equations.

Key Result

Theorem 1.1

Let $\beta\in(0,2]$ and $\alpha_s\in \left(0,2^{-8}r_0^4R^{-4}\right)$ if $\beta=2$. There exist positive constants $h_0$, $c_0$, $c_1$, $c_2$, $c_3$, $c_4$ depending on $\alpha_s$, $r_0$, and $R$ (with $h_0$ also depending on $\beta$ if $\beta\leq \frac{2}{3}$), such that for any $0<h<h_0$, we have

Theorems & Definitions (17)

  • Theorem 1.1
  • Remark 1.1
  • Remark 1.2
  • Remark 1.3
  • Theorem 1.2
  • Remark 1.4
  • Remark 2.1
  • Proposition 3.1
  • proof
  • Proposition 3.2
  • ...and 7 more