Abstract

We formulate the problem of finding equilibrium shapes of a thin inextensible elastic strip, developing further our previous work on the Mobius strip. By using the isometric nature of the deformation we reduce the variational problem to a second-order one-dimensional problem posed on the centreline of the strip. We derive Euler–Lagrange equations for this problem in Euler–Poincare form and formulate boundary-value problems for closed symmetric one- and two-sided strips. Numerical solutions for the Mobius strip show a singular point of stress localisation on the edge of the strip, a generic response of inextensible elastic sheets under torsional strain. By cutting and pasting operations on the Mobius strip solution, followed by parameter continuation, we construct equilibrium solutions for strips with different linking numbers and with multiple points of stress localisation. Solutions reveal how strips fold into planar or self-contacting shapes as the length-to-width ratio of the strip is decreased. Our results may be relevant for curvature effects on physical properties of extremely thin two-dimensional structures as for instance produced in nanostructured origami.

Highlights

  • We do not know who was the first to take a thin flexible strip of paper, to join its ends in space so thatB E.L

  • Gravesen & Willatzen [17] computed quantum eigenstates of a particle confined to the surface of a developable Möbius strip and compared their results with earlier calculations by Yakubo et al [62]

  • Approximate equations for deformations of wide strips were derived in the mid-1950s by Mansfield [34, 35]. These equations predict the distribution of generators of the developable surface while ignoring the actual three-dimensional geometry

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Summary

Introduction

We do not know who was the first to take a thin flexible strip of paper (papyrus, parchment, birch bark, animal skin, palm leaf or whatever material), to join its ends in space so that. Gravesen & Willatzen [17] computed quantum eigenstates of a particle confined to the surface of a developable Möbius strip and compared their results with earlier calculations by Yakubo et al [62]. They found curvature effects in the form of a splitting of the otherwise doubly degenerate ground state wave function (see [27]). Approximate equations for deformations of wide strips were derived in the mid-1950s by Mansfield [34, 35] These equations predict the distribution of generators of the developable surface while ignoring the actual three-dimensional geometry. We extend the work to closed one- and two-sided strips of different topology

Geometry of a Developable Strip
Edge of Regression
The Energy Functional
Variational Principle
Hamiltonian
Symmetries
Kinematics Equations
Full System of Equations
Properties of a One-Sided Strip
Boundary-Value Problem
Modified Boundary-Value Problem for Dn-Symmetric Solutions
Higher-Order One- and Two-Sided Developable Strips
Discussion
Two Special Cases
Full Text
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