Table of Contents
Fetching ...

Shape optimization under width constraint: the Cheeger constant and the torsional rigidity

Beniamin Bogosel

Abstract

In this article it is shown that the equilateral triangle maximizes the Cheeger constant and minimizes the torsional rigidity among shapes having a fixed minimal width. The proof techniques use direct comparisons with simpler shapes, consisting of disks with three disjoint caps. Comparison results for harmonic functions help establish that in non-equilateral configurations the shape derivative has an appropriate sign, contradicting optimality.

Shape optimization under width constraint: the Cheeger constant and the torsional rigidity

Abstract

In this article it is shown that the equilateral triangle maximizes the Cheeger constant and minimizes the torsional rigidity among shapes having a fixed minimal width. The proof techniques use direct comparisons with simpler shapes, consisting of disks with three disjoint caps. Comparison results for harmonic functions help establish that in non-equilateral configurations the shape derivative has an appropriate sign, contradicting optimality.

Paper Structure

This paper contains 6 sections, 12 theorems, 46 equations, 7 figures.

Key Result

Theorem 1

The equilateral triangle of unit minimal width minimizes the area among all planar convex shapes having unit minimal width.

Figures (7)

  • Figure 1: (left) Existence of a three-$r$-cap subset for a shape with given minimal width. (right) Example of a three-$r$-cap shape: convex hull of a disk $D_r$ of center $O$ and radius $r \in [1/3,1/2]$ and points $A,B,C$ such that $AO=BO=CO=1-r$.
  • Figure 2: A three-$r$-cap shape $T_{ABC}$ together with the arcs $\gamma_A, \gamma_B,\gamma_C$ near points $A,B,C$. In the figure, when $AB<AC$, the symmetric of the left part with respect to the vertical axis is contained in the right part.
  • Figure 3: Illustration for boundary conditions for $u_\theta, u_{\theta'}$ given by \ref{['eq:harmonic-slide']} for $\theta<\theta'$. Dirichlet boundary conditions $u_\theta=0$ and $u_{\theta'}=0$ hold everywhere on the boundary of the half-disk (including the diameter), except the arcs $\gamma_\gamma$ and $\gamma_{\theta'}$, respectively. On these arcs we have a boundary condition given by the same non-negative function $\phi$.
  • Figure 4: Geometric configuration for problem \ref{['eq:harmonic-K']} on the domain $K$, the convex hull of the half disk and a point $A$ on the real axis. The boundary condition is $u_\theta=0$ except an arc $\gamma_\theta$ which slides towards $A'$. Values of $u_\theta$ decrease in $\mathcal{C}_A$ as the positive boundary condition slides.
  • Figure 5: A three-$r$-cap shape with $AB<AC$ such that $A$ is on the positive real axis. The vertex $C$ is symmetrized with respect to the $x$-axis. The difference of the torsion function and its symmetrized will be compared in $\text{conv}(D_+,A)$.
  • ...and 2 more figures

Theorems & Definitions (16)

  • Theorem 1
  • Definition 2
  • Theorem 3
  • Conjecture 4
  • Theorem 5
  • Proposition 6
  • Proposition 7
  • Proposition 8
  • Proposition 9
  • Proposition 10
  • ...and 6 more