Inelastic mechanics: A unifying principle in biomechanics.
Many soft materials are classified as viscoelastic. They behave mechanically neither quite fluid-like nor quite solid-like - rather a bit of both. Biomaterials are often said to fall into this class. Here, we argue that this misses a crucial aspect, and that biomechanics is essentially damage mechanics, at heart. When deforming an animal cell or tissue, one can hardly avoid inducing the unfolding of protein domains, the unbinding of cytoskeletal crosslinkers, the breaking of weak sacrificial bonds, and the disruption of transient adhesions. We classify these activated structural changes as inelastic. They are often to a large degree reversible and are therefore not plastic in the proper sense, but they dissipate substantial amounts of elastic energy by structural damping. We review recent experiments involving biological materials on all scales, from single biopolymers over cells to model tissues, to illustrate the unifying power of this paradigm. A deliberately minimalistic yet phenomenologically very rich mathematical modeling framework for inelastic biomechanics is proposed. It transcends the conventional viscoelastic paradigm and suggests itself as a promising candidate for a unified description and interpretation of a wide range of experimental data. This article is part of a Special Issue entitled: Mechanobiology.
['Gralka|Matti|M|', 'Kroy|Klaus|K|']
D000818:Animals D002462:Cell Membrane D003599:Cytoskeleton D006801:Humans D008565:Membrane Proteins D008956:Models, Chemical D017434:Protein Structure, Tertiary
Inelastic biomechanics Cell aggregates Cytoskeleton Glassy wormlike chain In-vitro biopolymer networks Microrheology Rheological models Soft glassy rheology Structural plasticity Transient crosslinkers