How do fire ants control the rheology of their aggregations? A statistical mechanics approach
暂无分享,去创建一个
Tong Shen | Shankar Lalitha Sridhar | Franck J Vernerey | Robert J Wagner | F. Vernerey | R. J. Wagner | S. L. Sridhar | Tong Shen | Robert J. Wagner
[1] F. Vernerey,et al. A coupled Eulerian–Lagrangian extended finite element formulation for simulating large deformations in hyperelastic media with moving free boundaries , 2015 .
[2] Nathan J. Mlot,et al. Fire ants self-assemble into waterproof rafts to survive floods , 2011, Proceedings of the National Academy of Sciences.
[3] I. Couzin,et al. Collective memory and spatial sorting in animal groups. , 2002, Journal of theoretical biology.
[4] Craig W. Reynolds. Flocks, herds, and schools: a distributed behavioral model , 1987, SIGGRAPH.
[5] M. P. Stoykovich,et al. Remotely Triggered Locomotion of Hydrogel Mag-bots in Confined Spaces , 2017, Scientific Reports.
[6] E. Bonabeau,et al. Model of droplet dynamics in the Argentine ant Linepithema humile (Mayr) , 2001, Bulletin of mathematical biology.
[7] Mary C. Boyce,et al. Deformation of Elastomeric Networks: Relation between Molecular Level Deformation and Classical Statistical Mechanics Models of Rubber Elasticity , 2001 .
[8] F. Vernerey. Transient response of nonlinear polymer networks: A kinetic theory. , 2018, Journal of the mechanics and physics of solids.
[9] S. Rakshit,et al. Biomechanics of cell adhesion: how force regulates the lifetime of adhesive bonds at the single molecule level. , 2014, Physical chemistry chemical physics : PCCP.
[10] J. Deneubourg,et al. Cockroach aggregation based on strain odour recognition , 2004, Animal Behaviour.
[11] S. Rakshit,et al. Ideal, catch, and slip bonds in cadherin adhesion , 2012, Proceedings of the National Academy of Sciences.
[12] T. Vicsek,et al. Spontaneously ordered motion of self-propelled particles , 1997, cond-mat/0611741.
[13] S. Bryant,et al. Tuning tissue growth with scaffold degradation in enzyme-sensitive hydrogels: a mathematical model. , 2016, Soft matter.
[14] P. Hänggi,et al. Reaction-rate theory: fifty years after Kramers , 1990 .
[15] H. Chaté,et al. Collective motion of self-propelled particles interacting without cohesion. , 2007, Physical review. E, Statistical, nonlinear, and soft matter physics.
[16] E. Altshuler,et al. Entangled active matter: From cells to ants , 2016 .
[17] Tarek I. Zohdi,et al. Mechanistic modeling of swarms , 2009 .
[18] Tarek I. Zohdi,et al. An agent-based computational framework for simulation of competing hostile planet-wide populations , 2017 .
[19] David Hu,et al. Mechanics of fire ant aggregations. , 2016, Nature materials.
[20] F. Vernerey,et al. Statistical Damage Mechanics of Polymer Networks. , 2018, Macromolecules.
[21] Radhika Nagpal,et al. Designing Collective Behavior in a Termite-Inspired Robot Construction Team , 2014, Science.
[22] T. Vicsek,et al. Collective Motion , 1999, physics/9902023.
[23] Sachit Butail,et al. Zebrafish response to 3D printed shoals of conspecifics: the effect of body size , 2016, Bioinspiration & biomimetics.
[24] F. Vernerey,et al. The Chain Distribution Tensor: Linking Nonlinear Rheology and Chain Anisotropy in Transient Polymers , 2018, Polymers.
[25] P. Hogeweg,et al. Modelling Morphogenesis: From Single Cells to Crawling Slugs. , 1997, Journal of theoretical biology.
[26] F. Vernerey,et al. Computational modeling of the large deformation and flow of viscoelastic polymers , 2018, Computational mechanics.
[27] Massimo Fornasier,et al. Particle, kinetic, and hydrodynamic models of swarming , 2010 .
[28] Nathan J. Mlot,et al. Fire ants perpetually rebuild sinking towers , 2017, Royal Society Open Science.
[29] F. Vernerey,et al. The mechanics of hydrogel crawlers in confined environment , 2017, Journal of The Royal Society Interface.
[30] F. Tanaka,et al. Viscoelastic properties of physically crosslinked networks: Part 2. Dynamic mechanical moduli , 1992 .
[31] D C Krakauer,et al. Spatial scales of desert locust gregarization. , 1998, Proceedings of the National Academy of Sciences of the United States of America.
[32] P. Nott,et al. The collective dynamics of self-propelled particles , 2007, Journal of Fluid Mechanics.
[33] T. Indei. Necessary conditions for shear thickening in associating polymer networks , 2007 .
[34] Vicsek,et al. Novel type of phase transition in a system of self-driven particles. , 1995, Physical review letters.
[35] A. Bertozzi,et al. Self-propelled particles with soft-core interactions: patterns, stability, and collapse. , 2006, Physical review letters.
[36] Radhika Nagpal,et al. Programmable self-assembly in a thousand-robot swarm , 2014, Science.
[37] S. Bryant,et al. Heterogeneity is key to hydrogel-based cartilage tissue regeneration. , 2017, Soft matter.
[38] A. Fernández-Nieves,et al. Activity-driven changes in the mechanical properties of fire ant aggregations. , 2017, Physical review. E.
[39] Dirk Helbing,et al. Simulating dynamical features of escape panic , 2000, Nature.
[40] F. Vernerey,et al. Role of catch bonds in actomyosin mechanics and cell mechanosensitivity. , 2016, Physical review. E.
[41] Tarek I. Zohdi,et al. Computational design of swarms , 2003 .
[42] F. Vernerey,et al. A statistically-based continuum theory for polymers with transient networks , 2017 .
[43] Paul C Foster,et al. Fire ants actively control spacing and orientation within self-assemblages , 2014, Journal of Experimental Biology.