TY - JOUR
T1 - How Cross-Link Numbers Shape the Large-Scale Physics of Cytoskeletal Materials
AU - Furthauer, Sebastian
AU - Shelley, Michael J.
N1 - Publisher Copyright:
© 2022 Annual Reviews Inc.. All rights reserved.
PY - 2022
Y1 - 2022
N2 - Cytoskeletal networks are the main actuators of cellular mechanics, and a foundational example for active matter physics. In cytoskeletal networks, motion is generated on small scales by filaments that push and pull on each other via molecular-scale motors. These local actuations give rise to large-scale stresses and motion. To understand how microscopic processes can give rise to self-organized behavior on larger scales it is important to consider what mechanisms mediate long-ranged mechanical interactions in the systems. Two scenarios have been considered in the recent literature. The first scenario is systems that are relatively sparse, in which most of the large-scale momentum transfer is mediated by the solvent in which cytoskeletal filaments are suspended. The second scenario is systems in which filaments are coupled via cross-link molecules throughout. Here, we review the differences and commonalities between the physics of these two regimes. We also survey the literature for the numbers that allow us to place a material within either of these two classes.
AB - Cytoskeletal networks are the main actuators of cellular mechanics, and a foundational example for active matter physics. In cytoskeletal networks, motion is generated on small scales by filaments that push and pull on each other via molecular-scale motors. These local actuations give rise to large-scale stresses and motion. To understand how microscopic processes can give rise to self-organized behavior on larger scales it is important to consider what mechanisms mediate long-ranged mechanical interactions in the systems. Two scenarios have been considered in the recent literature. The first scenario is systems that are relatively sparse, in which most of the large-scale momentum transfer is mediated by the solvent in which cytoskeletal filaments are suspended. The second scenario is systems in which filaments are coupled via cross-link molecules throughout. Here, we review the differences and commonalities between the physics of these two regimes. We also survey the literature for the numbers that allow us to place a material within either of these two classes.
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U2 - 10.1146/annurev-conmatphys-052521-093943
DO - 10.1146/annurev-conmatphys-052521-093943
M3 - Review article
AN - SCOPUS:85127235543
SN - 1947-5454
VL - 13
SP - 365
EP - 384
JO - Annual Review of Condensed Matter Physics
JF - Annual Review of Condensed Matter Physics
ER -