Newton's problem of minimal resistance under the single-impact assumption
Alexander Plakhov

TL;DR
This paper extends Newton's minimal resistance problem to a broader class of bodies under the single-impact condition, providing analytical solutions and demonstrating significant resistance reduction, with the infimum of resistance being zero for even more general cases.
Contribution
It generalizes Newton's classical problem by removing convexity and symmetry constraints, solving for bodies with SIC, and analyzing resistance reduction and infimum in wider classes.
Findings
Resistance can be reduced more than twofold compared to Newton's original solution.
The resistance ratio approaches 2 as M approaches 0 and 81/4 as M approaches infinity.
The infimum of resistance is zero for bodies with both single and double impacts.
Abstract
A parallel flow of non-interacting point particles is incident on a body at rest. When hitting the body's surface, the particles are reflected elastically. Assume that each particle hits the body at most once (SIC condition); then the force of resistance of the body along the flow direction can be written down in a simple analytical form. The problem of minimal resistance within this model was first considered by Newton (1687) in the class of bodies with a fixed length M along the flow direction and with a fixed maximum orthogonal cross section, under the additional conditions that the body is convex and rotationally symmetric. Here we solve the problem (first stated by Ferone, Buttazzo, and Kawohl in 1995) for the wider class of bodies satisfying SIC and with the additional conditions removed. The scheme of solution is inspired by Besicovitch's method of solving the Kakeya problem.…
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