Static Equilibria of Perturbed Spheres: A Single-Harmonic Class Map, a Parity Obstruction, and a Certified Counter for the Mono-Monostatic Regime
arXiv:2608.11213
Abstract
Varkonyi and Domokos proved that homogeneous convex bodies exist with any prescribed numbers of stable and of unstable static equilibria, the case being the mono-monostatic Gomboc. Their result is an existence statement. We give a complete constructive answer for the simplest nondegenerate shapes: a homogeneous body whose boundary is the unit sphere perturbed radially by a single real spherical harmonic (, ) has exactly stable and unstable equilibria, for every amplitude in the convex range when and for small amplitude when . For the reduction to the critical points of the harmonic is an identity: the symmetry of a single tesseral harmonic pins the centroid at the origin exactly, so the centroid-to-surface distance is a strictly increasing function of the harmonic. We count the critical points of and verify the Poincare-Hopf balance in index form, the polar monkey-saddles persisting unsplit with index . Three consequences follow: a single harmonic populates only the diagonal , so none of degree is mono-monostatic; any centrally symmetric (even-degree) perturbation has even , a parity obstruction; hence mono-monostaticity is intrinsically multi-harmonic. A predict-then-confirm study on eight bodies matches the formula exactly. For the multi-harmonic regime, where mono-monostatic bodies live, we give a certified equilibrium counter (interval arithmetic on the centroid-to-surface distance, Krawczyk uniqueness, interval-Hessian classification, stereographic polar charts) that, given the centroid, provably neither under- nor over-counts. It certifies specific near-spherical bodies mono-monostatic, including a known analytic parameterization, settling by certified computation a question that drainage-basin and seed-based methods leave ambiguous.
10 pages, 1 figure