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Published on: June 6, 2020
Geometry and the onset of rigidity in a disordered network
Mathijs F J Vermeulen1, Anwesha Bose1, Cornelis Storm1,2
1Department of Applied Physics, Eindhoven University of Technology, Den Dolech 2, 5600 MB Eindhoven, Netherlands.
Undercoordinated disordered spring networks can suddenly become rigid under strain. This geometric rigidity transition, not predicted by standard analyses, is linked to the emergence of a single self-stress state and a floppy mode.
Area of Science:
- * Physics
- * Materials Science
- * Network Mechanics
Background:
- * Disordered spring networks exhibit undercoordination, making them susceptible to abrupt rigidity changes under applied strain.
- * Traditional mechanical analyses (e.g., Maxwell-Calladine count, pebble game) fail to predict or characterize these geometric rigidity transitions.
- * The underlying cause of this rigidity is geometric, not solely dependent on network topology (nodes and bonds).
Purpose of the Study:
- * To investigate the geometric origin of rigidity transitions in undercoordinated disordered spring networks.
- * To apply topological analysis tools to predict and characterize these transitions in 2D random spring networks.
- * To understand the mechanical behavior and elastic properties of networks beyond the critical strain.
Main Methods:
- * Application of topological analysis tools for zero modes and states of self-stress, adapted from regular lattices.
- * Analysis of 2D random spring networks subjected to finite simple shear strain.
- * Use of singular value decomposition on the network's compatibility matrix in the subcritical regime.
Main Results:
- * Rigidity onset at a critical shear strain (γ*) coincides with the appearance of one state of self-stress and one floppy mode.
- * The transition conserves the topological invariant difference between zero modes and self-stress states.
- * Networks develop a finite shear modulus and anisotropic elastic properties post-transition, with enhanced resistance to deformation along the shear direction.
- * Critical scaling of the differential shear modulus is confirmed.
- * A vanishing singular value in the compatibility matrix foreshadows the rigidity onset.
Conclusions:
- * Geometric factors, not just network topology, govern rigidity transitions in disordered spring networks.
- * Topological analysis tools can predict and characterize these transitions, revealing the interplay of self-stress and floppy modes.
- * The study provides a framework for understanding the anisotropic mechanical response of networks after rigidification.
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