Applications of the Kosambi–Cartan–Chern Theory to Hamiltonian Systems on a Cotangent Bundle: Linking Geometric Quantities to the Self-Similar Motions of Three Point Vortices

This study presents a differential geometric framework for Hamiltonian systems expressed in terms of first-order differential equations. For systems governed by second-order ordinary differential equations on tangent bundles, such as Euler–Lagrange systems, the stability of trajectories under pertur...

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Main Authors: Yuma Hirakui, Takahiro Yajima
Format: Article
Language:English
Published: MDPI AG 2024-12-01
Series:Mathematics
Subjects:
Online Access:https://www.mdpi.com/2227-7390/13/1/126
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author Yuma Hirakui
Takahiro Yajima
author_facet Yuma Hirakui
Takahiro Yajima
author_sort Yuma Hirakui
collection DOAJ
description This study presents a differential geometric framework for Hamiltonian systems expressed in terms of first-order differential equations. For systems governed by second-order ordinary differential equations on tangent bundles, such as Euler–Lagrange systems, the stability of trajectories under perturbations is analyzed based on the eigenvalue of the deviation curvature tensor. Building upon this Jacobi stability analysis approach, four geometric quantities for Hamiltonian systems are derived considering perturbations to trajectories on a cotangent bundle. As a specific Hamiltonian system, a hydrodynamic three-point vortex system is examined, and its four geometric quantities are computed using the Hamiltonian equation. The eigenvalues of these geometric quantities are then used to classify the divergent and collapsing trajectories of point vortices. Specifically, for the divergent trajectories of vortices, the eigenvalues of the geometric quantities converge to zero over time. Conversely, for their collapsing trajectories, the eigenvalues increase with time. This result implies that at the point of vortex collapse, the system becomes geometrically unstable, with diverging trajectory perturbations.
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spelling doaj-art-e584e4fd33eb467cbab0d73f6d2b4a9a2025-01-10T13:18:19ZengMDPI AGMathematics2227-73902024-12-0113112610.3390/math13010126Applications of the Kosambi–Cartan–Chern Theory to Hamiltonian Systems on a Cotangent Bundle: Linking Geometric Quantities to the Self-Similar Motions of Three Point VorticesYuma Hirakui0Takahiro Yajima1Division of Advanced Transdisciplinary Science, Graduate School of Regional Development and Creativity, Utsunomiya University, Utsunomiya 321-8585, JapanMechanical Systems Engineering Course, Department of Fundamental Engineering, School of Engineering, Utsunomiya University, Utsunomiya 321-8585, JapanThis study presents a differential geometric framework for Hamiltonian systems expressed in terms of first-order differential equations. For systems governed by second-order ordinary differential equations on tangent bundles, such as Euler–Lagrange systems, the stability of trajectories under perturbations is analyzed based on the eigenvalue of the deviation curvature tensor. Building upon this Jacobi stability analysis approach, four geometric quantities for Hamiltonian systems are derived considering perturbations to trajectories on a cotangent bundle. As a specific Hamiltonian system, a hydrodynamic three-point vortex system is examined, and its four geometric quantities are computed using the Hamiltonian equation. The eigenvalues of these geometric quantities are then used to classify the divergent and collapsing trajectories of point vortices. Specifically, for the divergent trajectories of vortices, the eigenvalues of the geometric quantities converge to zero over time. Conversely, for their collapsing trajectories, the eigenvalues increase with time. This result implies that at the point of vortex collapse, the system becomes geometrically unstable, with diverging trajectory perturbations.https://www.mdpi.com/2227-7390/13/1/126KCC theoryHamiltonian systempoint vortexcotangent bundle
spellingShingle Yuma Hirakui
Takahiro Yajima
Applications of the Kosambi–Cartan–Chern Theory to Hamiltonian Systems on a Cotangent Bundle: Linking Geometric Quantities to the Self-Similar Motions of Three Point Vortices
Mathematics
KCC theory
Hamiltonian system
point vortex
cotangent bundle
title Applications of the Kosambi–Cartan–Chern Theory to Hamiltonian Systems on a Cotangent Bundle: Linking Geometric Quantities to the Self-Similar Motions of Three Point Vortices
title_full Applications of the Kosambi–Cartan–Chern Theory to Hamiltonian Systems on a Cotangent Bundle: Linking Geometric Quantities to the Self-Similar Motions of Three Point Vortices
title_fullStr Applications of the Kosambi–Cartan–Chern Theory to Hamiltonian Systems on a Cotangent Bundle: Linking Geometric Quantities to the Self-Similar Motions of Three Point Vortices
title_full_unstemmed Applications of the Kosambi–Cartan–Chern Theory to Hamiltonian Systems on a Cotangent Bundle: Linking Geometric Quantities to the Self-Similar Motions of Three Point Vortices
title_short Applications of the Kosambi–Cartan–Chern Theory to Hamiltonian Systems on a Cotangent Bundle: Linking Geometric Quantities to the Self-Similar Motions of Three Point Vortices
title_sort applications of the kosambi cartan chern theory to hamiltonian systems on a cotangent bundle linking geometric quantities to the self similar motions of three point vortices
topic KCC theory
Hamiltonian system
point vortex
cotangent bundle
url https://www.mdpi.com/2227-7390/13/1/126
work_keys_str_mv AT yumahirakui applicationsofthekosambicartancherntheorytohamiltoniansystemsonacotangentbundlelinkinggeometricquantitiestotheselfsimilarmotionsofthreepointvortices
AT takahiroyajima applicationsofthekosambicartancherntheorytohamiltoniansystemsonacotangentbundlelinkinggeometricquantitiestotheselfsimilarmotionsofthreepointvortices