Two-scale geometric modelling for defective media: An approach using fibre bundles

A new geometrically exact micro-structured model is constructed in order to propose a generalisation of the notion of Riemann–Cartan manifolds. The construction is done using the theory of affine bundles, Ehresmann connections, and solder forms. This model is based on the concept of two different length scales: a macroscopic scale—a manifold <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi mathvariant="double-struck">B</mml:mi> </mml:mrow> </mml:math> of dimension 1, 2, or 3—and a microscopic scale—an affine space <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="script">B</mml:mi> </mml:mrow> <mml:mrow> <mml:mover accent="false"> <mml:mrow> <mml:mi>x</mml:mi> </mml:mrow> <mml:mo>¯</mml:mo> </mml:mover> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> of dimension 3 at each <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mover accent="false"> <mml:mrow> <mml:mi>x</mml:mi> </mml:mrow> <mml:mo>¯</mml:mo> </mml:mover> <mml:mo>∈</mml:mo> <mml:mi mathvariant="double-struck">B</mml:mi> </mml:mrow> </mml:math> . As they interact with each other, they produce emergent behaviours such as dislocations (torsion) and disclinations (curvature). A first-order placement map <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi mathvariant="bold">F</mml:mi> <mml:mo>:</mml:mo> <mml:mi mathvariant="normal">T</mml:mi> <mml:mi mathvariant="script">B</mml:mi> <mml:mo stretchy="false">→</mml:mo> <mml:mi mathvariant="normal">T</mml:mi> <mml:mi mathvariant="script">E</mml:mi> </mml:mrow> </mml:math> between a micro-structured body <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi mathvariant="script">B</mml:mi> </mml:mrow> </mml:math> and the micro-structured ambient space <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi mathvariant="script">E</mml:mi> </mml:mrow> </mml:math> is constructed, allowing to pull back the ambient geometry onto the body <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi mathvariant="script">B</mml:mi> </mml:mrow> </mml:math> . In order to allow for curvature to arise, F is, in general, not required to be a gradient. Central to this model is the new notion of compatible pseudo-metric, providing, in addition to a macroscopic metric (the usual Cauchy–Green tensor) and a microscopic metric, a notion of coupling between the microscopic and macroscopic realms. A notion of frame indifference is formalised and invariants are computed. In the case of a micro-linear structure, it is shown that the data of these invariants are equivalent to the data of the pseudo-metric.

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Publication Details

Journal
Mathematics and Mechanics of Solids
Published
2025-06-17
DOI
https://doi.org/10.1177/10812865241312135
Citations
2
Primary Topic
Nonlocal and gradient elasticity in micro/nano structures
Type
article
Field-Weighted Citation Impact
1.04

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article

Two-scale geometric modelling for defective media: An approach using fibre bundles

Guy Casale, Loïc Le Marrec, Mewen Crespo
2 citations
Mathematics and Mechanics of Solids
Nonlocal and gradient elasticity in micro/nano structures
1.04
article

Two-scale geometric modelling for defective media: An approach using fibre bundles

Guy Casale, Loïc Le Marrec, Mewen Crespo
article en
2 citations

Abstract

A new geometrically exact micro-structured model is constructed in order to propose a generalisation of the notion of Riemann–Cartan manifolds. The construction is done using the theory of affine bundles, Ehresmann connections, and solder forms. This model is based on the concept of two different length scales: a macroscopic scale—a manifold <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi mathvariant="double-struck">B</mml:mi> </mml:mrow> </mml:math> of dimension 1, 2, or 3—and a microscopic scale—an affine space <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="script">B</mml:mi> </mml:mrow> <mml:mrow> <mml:mover accent="false"> <mml:mrow> <mml:mi>x</mml:mi> </mml:mrow> <mml:mo>¯</mml:mo> </mml:mover> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> of dimension 3 at each <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mover accent="false"> <mml:mrow> <mml:mi>x</mml:mi> </mml:mrow> <mml:mo>¯</mml:mo> </mml:mover> <mml:mo>∈</mml:mo> <mml:mi mathvariant="double-struck">B</mml:mi> </mml:mrow> </mml:math> . As they interact with each other, they produce emergent behaviours such as dislocations (torsion) and disclinations (curvature). A first-order placement map <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi mathvariant="bold">F</mml:mi> <mml:mo>:</mml:mo> <mml:mi mathvariant="normal">T</mml:mi> <mml:mi mathvariant="script">B</mml:mi> <mml:mo stretchy="false">→</mml:mo> <mml:mi mathvariant="normal">T</mml:mi> <mml:mi mathvariant="script">E</mml:mi> </mml:mrow> </mml:math> between a micro-structured body <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi mathvariant="script">B</mml:mi> </mml:mrow> </mml:math> and the micro-structured ambient space <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi mathvariant="script">E</mml:mi> </mml:mrow> </mml:math> is constructed, allowing to pull back the ambient geometry onto the body <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi mathvariant="script">B</mml:mi> </mml:mrow> </mml:math> . In order to allow for curvature to arise, F is, in general, not required to be a gradient. Central to this model is the new notion of compatible pseudo-metric, providing, in addition to a macroscopic metric (the usual Cauchy–Green tensor) and a microscopic metric, a notion of coupling between the microscopic and macroscopic realms. A notion of frame indifference is formalised and invariants are computed. In the case of a micro-linear structure, it is shown that the data of these invariants are equivalent to the data of the pseudo-metric.

Mathematics and Mechanics of Solids
Centre National de la Recherche Scientifique (FR), Institut de recherche mathématique de Rennes (FR), Université de Rennes (FR)
Centre Henri Lebesgue
Openalex Percentile: Top 24%
Nonlocal and gradient elasticity in micro/nano structures
1.04
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