Klein-Arnold tensegrities

Fuente: arXiv
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Autores principales: Karpenkov, Oleg, Mohammadi, Fatemeh, Müller, Christian, Schulze, Bernd
Formato: Preprint
Publicado: 2024
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author Karpenkov, Oleg
Mohammadi, Fatemeh
Müller, Christian
Schulze, Bernd
author_facet Karpenkov, Oleg
Mohammadi, Fatemeh
Müller, Christian
Schulze, Bernd
contents In this paper, we introduce new classes of infinite and combinatorially periodic tensegrities, derived from algebraic multidimensional continued fractions in the sense of F. Klein. We describe the stress coefficients on edges through integer invariants of these continued fractions, as initiated by V.I. Arnold, thereby creating a novel connection between geometric rigidity theory and the geometry of continued fractions. Remarkably, the new classes of tensegrities possess rational self-stress coefficients. To establish the self-stressability of the frameworks, we present a projective version of the classical Maxwell-Cremona lifting principle, a result of independent interest.
format Preprint
id arxiv_https___arxiv_org_abs_2410_12729
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Klein-Arnold tensegrities
Karpenkov, Oleg
Mohammadi, Fatemeh
Müller, Christian
Schulze, Bernd
Combinatorics
Metric Geometry
In this paper, we introduce new classes of infinite and combinatorially periodic tensegrities, derived from algebraic multidimensional continued fractions in the sense of F. Klein. We describe the stress coefficients on edges through integer invariants of these continued fractions, as initiated by V.I. Arnold, thereby creating a novel connection between geometric rigidity theory and the geometry of continued fractions. Remarkably, the new classes of tensegrities possess rational self-stress coefficients. To establish the self-stressability of the frameworks, we present a projective version of the classical Maxwell-Cremona lifting principle, a result of independent interest.
title Klein-Arnold tensegrities
topic Combinatorics
Metric Geometry
url https://arxiv.org/abs/2410.12729