Energy function of 2D and 3D coarse systems

In this work, while using the Flow Curvature Method developed by one of us (JMG), we prove that the energy function of two and three-dimensional coarse systems involving a small parameter μ can be directly deduced from the curvature of their trajectory curves when μ tends to zero. Such a result thus confirms the relationship between curvature and energy function for a certain class of differential systems already established in one of our previous contributions. Then, we state that the rate of change of the energy function of such coarse systems is equal to the scalar product of the velocity vector field and its first time derivative, i.e. the acceleration vector field . The comparison of these results with the so-called Frénet frame enables to prove that energy function is proportional to the normal component of the acceleration when μ tends to zero while the rate of change of the energy function is proportional to the tangential component of the acceleration at first order in μ . Two and three-dimensional examples are then used to emphasize these two main results.

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Publication Details

Journal
Chaos Solitons & Fractals
Published
2025-06-13
DOI
https://doi.org/10.1016/j.chaos.2025.116643
Citations
1
Primary Topic
Theoretical and Computational Physics
Type
article
Field-Weighted Citation Impact
1.26

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article

Energy function of 2D and 3D coarse systems

Jean‐Marc Ginoux, R. Meucci, Jaume Llibre, Julien Clinton Sprott
1 citations
Chaos Solitons & Fractals
Theoretical and Computational Physics
1.26
article

Energy function of 2D and 3D coarse systems

Jean‐Marc Ginoux, R. Meucci, Jaume Llibre, Julien Clinton Sprott
article en
1 citations

Abstract

In this work, while using the Flow Curvature Method developed by one of us (JMG), we prove that the energy function of two and three-dimensional coarse systems involving a small parameter μ can be directly deduced from the curvature of their trajectory curves when μ tends to zero. Such a result thus confirms the relationship between curvature and energy function for a certain class of differential systems already established in one of our previous contributions. Then, we state that the rate of change of the energy function of such coarse systems is equal to the scalar product of the velocity vector field and its first time derivative, i.e. the acceleration vector field . The comparison of these results with the so-called Frénet frame enables to prove that energy function is proportional to the normal component of the acceleration when μ tends to zero while the rate of change of the energy function is proportional to the tangential component of the acceleration at first order in μ . Two and three-dimensional examples are then used to emphasize these two main results.

Chaos Solitons & FractalsVol. 199
Universitat Autònoma de Barcelona (ES), Centre National de la Recherche Scientifique (FR), University of Wisconsin System (US), University of Wisconsin–Madison (US), Université de Toulon (FR), Laboratoire d’Informatique et Systèmes (FR)
Generalitat de Catalunya, Agència de Gestió d'Ajuts Universitaris i de Recerca, Agencia Estatal de Investigación, Spanish National Plan for Scientific and Technical Research and Innovation
Affordable and clean energy
Openalex Percentile: Top 21%
Theoretical and Computational Physics
1.26
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