English

On the structure of singular points of a solution to Newton's least resistance problem

Optimization and Control 2022-03-29 v1 Metric Geometry

Abstract

We consider the following problem stated in 1993 by Buttazzo and Kawohl: minimize the functional  ⁣ ⁣Ω(1+u(x,y)2)1dxdy\int\!\!\int_\Omega (1 + |\nabla u(x,y)|^2)^{-1} dx\, dy in the class of concave functions u:Ω[0,M]u: \Omega \to [0,M], where ΩR2\Omega \subset \mathbb{R}^2 is a convex domain and M>0M > 0. It generalizes the classical minimization problem, which was initially stated by I. Newton in 1687 in the more restricted class of radial functions. The problem is not solved until now; there is even nothing known about the structure of singular points of a solution. In this paper we, first, solve a family of auxiliary 2D least resistance problems and, second, apply the obtained results to study singular points of a solution to our original problem. More precisely, we derive a necessary condition for a point being a ridge singular point of a solution and prove, in particular, that all ridge singular points with horizontal edge lie on the top level and zero level sets.

Keywords

Cite

@article{arxiv.2203.14235,
  title  = {On the structure of singular points of a solution to Newton's least resistance problem},
  author = {Alexander Plakhov},
  journal= {arXiv preprint arXiv:2203.14235},
  year   = {2022}
}

Comments

14 pages, 6 figures