Golden Ratio Thresholds in Near-Newtonian Orbit Closure — E8 Intelligence Research

FINDING: Bertrand's theorem strictly limits closed orbits to inverse-square and Hooke's-law potentials; a perturbative analysis reveals golden-ratio-linked eccentricity thresholds for orbit closure in near-Newtonian systems. | MATH: Bertrand's theorem: closed, bounded orbits exist only for \(V(r) \propto -1/r\) (Kepler) and \(V(r) \propto r^2\) (harmonic oscillator). For a general central potential \(V(r) = -k/r^{n}\), closure requires \(n = 1\) (Kepler) or \(n = -2\) (Hooke). Precession angle per orbit: \(\Delta \phi = 2\pi \left( \frac{1}{\sqrt{3 - n}} - 1 \right)\) for small perturbations about circular orbits. For \(n = 1 + \epsilon\), the apsidal precession per revolution is \(\Delta \omega = \pi \epsilon\) (first order). The arXiv paper (1711.10119) explicitly constructs elliptical orbits under perturbations and finds that the eccentricity \(e\) of a closed orbit under a small \(1/r^3\) perturbation satisfies \(e^2 = 1 - \frac{2}{3} \approx 0.333\), and the ratio of radial to ang Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-10-24
DOI
https://doi.org/10.5281/zenodo.23610169
Primary Topic
Advanced Mathematical Theories and Applications
Type
preprint
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Golden Ratio Thresholds in Near-Newtonian Orbit Closure — E8 Intelligence Research

Andrew Stewart Caldin
Zenodo (CERN European Organization for Nuclear Research)
Advanced Mathematical Theories and Applications
preprint

Golden Ratio Thresholds in Near-Newtonian Orbit Closure — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: Bertrand's theorem strictly limits closed orbits to inverse-square and Hooke's-law potentials; a perturbative analysis reveals golden-ratio-linked eccentricity thresholds for orbit closure in near-Newtonian systems. | MATH: Bertrand's theorem: closed, bounded orbits exist only for \(V(r) \propto -1/r\) (Kepler) and \(V(r) \propto r^2\) (harmonic oscillator). For a general central potential \(V(r) = -k/r^{n}\), closure requires \(n = 1\) (Kepler) or \(n = -2\) (Hooke). Precession angle per orbit: \(\Delta \phi = 2\pi \left( \frac{1}{\sqrt{3 - n}} - 1 \right)\) for small perturbations about circular orbits. For \(n = 1 + \epsilon\), the apsidal precession per revolution is \(\Delta \omega = \pi \epsilon\) (first order). The arXiv paper (1711.10119) explicitly constructs elliptical orbits under perturbations and finds that the eccentricity \(e\) of a closed orbit under a small \(1/r^3\) perturbation satisfies \(e^2 = 1 - \frac{2}{3} \approx 0.333\), and the ratio of radial to ang Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Zenodo (CERN European Organization for Nuclear Research)
Advanced Mathematical Theories and Applications
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