Learning to school in the presence of hydrodynamic interactions

Schooling, an archetype of collective behaviour, emerges from the interactions of fish responding to sensory information mediated by their aqueous environment. A fundamental and largely unexplored question in fish schooling concerns the role of hydrodynamics. Here, we investigate this question by modelling swimmers as vortex dipoles whose interactions are governed by the Biot–Savart law. When we enhance these dipoles with behavioural rules from classical agent-based models, we find that they do not lead robustly to schooling because of flow-mediated interactions. We therefore propose to use swimmers equipped with adaptive decision-making that adjust their gaits through a reinforcement learning algorithm in response to nonlinearly varying hydrodynamic loads. We demonstrate that these swimmers can maintain their relative position within a formation by adapting their strength and school in a variety of prescribed geometrical arrangements. Furthermore, we identify schooling patterns that minimize the individual and collective swimming effort, through an evolutionary optimization. The present work suggests that the adaptive response of individual swimmers to flow-mediated interactions is critical in fish schooling.

[1]  I. Couzin,et al.  Collective memory and spatial sorting in animal groups. , 2002, Journal of theoretical biology.

[2]  Peter Dayan,et al.  Q-learning , 1992, Machine Learning.

[3]  Zbigniew Michalewicz,et al.  Evolutionary Optimization , 2012, Variants of Evolutionary Algorithms for Real-World Applications.

[4]  J. Blake,et al.  Collective Hydrodynamics of Swimming Microorganisms : Living Fluids , 2012 .

[5]  Hiro-Sato Niwa Self-organizing Dynamic Model of Fish Schooling , 1994 .

[6]  Craig W. Reynolds Flocks, herds, and schools: a distributed behavioral model , 1987, SIGGRAPH.

[7]  Sriram Ramaswamy,et al.  Hydrodynamic fluctuations and instabilities in ordered suspensions of self-propelled particles. , 2001, Physical review letters.

[8]  Jean-Luc Thiffeault,et al.  Stirring by squirmers , 2010, Journal of Fluid Mechanics.

[9]  A. Smits,et al.  Propulsive performance of unsteady tandem hydrofoils in an in-line configuration , 2014 .

[10]  P. Koumoutsakos,et al.  1 Supplementary Information : Optimal morphokinematics for undulatory swimmers at intermediate Reynolds numbers , 2015 .

[11]  P. Koumoutsakos,et al.  Simulations of optimized anguilliform swimming , 2006, Journal of Experimental Biology.

[12]  Petros Koumoutsakos,et al.  Reducing the Time Complexity of the Derandomized Evolution Strategy with Covariance Matrix Adaptation (CMA-ES) , 2003, Evolutionary Computation.

[13]  C. Breder Vortices and fish schools , 1965 .

[14]  Petros Koumoutsakos,et al.  C-start: optimal start of larval fish , 2012, Journal of Fluid Mechanics.

[15]  Lakshminarayanan Mahadevan,et al.  Planar controlled gliding, tumbling and descent , 2011, Journal of Fluid Mechanics.

[16]  Steven V. Viscido,et al.  Self-Organized Fish Schools: An Examination of Emergent Properties , 2002, The Biological Bulletin.

[17]  P. Koumoutsakos,et al.  Optimal shapes for anguilliform swimmers at intermediate Reynolds numbers , 2013, Journal of Fluid Mechanics.

[18]  Kurihara,et al.  Three-dimensional Structure , 2006 .

[19]  P. Colgan,et al.  Fish schools and their hydrodynamic function: a reanalysis , 1987, Environmental Biology of Fishes.

[20]  Takuji Ishikawa,et al.  Hydrodynamic interaction of two swimming model micro-organisms , 2006, Journal of Fluid Mechanics.

[21]  Petros Koumoutsakos,et al.  Flow mediated interactions between two cylinders at finite Re numbers , 2012 .

[22]  J. Terborgh,et al.  Oddity and the ‘confusion effect’ in predation , 1986, Animal Behaviour.

[23]  G. Lauder,et al.  Fish Exploiting Vortices Decrease Muscle Activity , 2003, Science.

[24]  I. Aoki A simulation study on the schooling mechanism in fish. , 1982 .

[25]  Eva Kanso,et al.  Hydrodynamically coupled rigid bodies , 2007, Journal of Fluid Mechanics.

[26]  Lailai Zhu,et al.  Self-propulsion in viscoelastic fluids: Pushers vs. pullers , 2012, 1212.0123.

[27]  Jun Zhang,et al.  Anomalous hydrodynamic drafting of interacting flapping flags. , 2008, Physical review letters.

[28]  Simon Hubbard,et al.  A model of the formation of fish schools and migrations of fish , 2004 .

[29]  R. Barnes,et al.  An introduction to marine ecology , 1982 .

[30]  J. Périaux,et al.  EVOLUTIONARY OPTIMIZATION OF SCALAR TRANSPORT IN CYLINDER ARRAYS ON MULTIGPU/MULTICORE ARCHITECTURES , 2011 .

[31]  T. Pitcher,et al.  The three-dimensional structure of fish schools , 1980, Behavioral Ecology and Sociobiology.

[32]  Peter Dayan,et al.  Technical Note: Q-Learning , 2004, Machine Learning.

[33]  Charles Meneveau,et al.  The flow field around a freely swimming copepod in steady motion. Part I: Theoretical analysis , 2002 .

[34]  M. Gazzola Simulation, optimization and learning of artificial swimmers , 2013 .

[35]  John O Dabiri,et al.  Fish schooling as a basis for vertical axis wind turbine farm design , 2010, Bioinspiration & biomimetics.

[36]  I. Couzin,et al.  Effective leadership and decision-making in animal groups on the move , 2005, Nature.

[37]  Petros Koumoutsakos,et al.  Simulations of single and multiple swimmers with non-divergence free deforming geometries , 2011, J. Comput. Phys..

[38]  Donald L. Koch,et al.  Collective Hydrodynamics of Swimming Microorganisms: Living Fluids , 2011 .

[39]  Richard S. Sutton,et al.  Reinforcement Learning: An Introduction , 1998, IEEE Trans. Neural Networks.

[40]  John F. Brady,et al.  STOKESIAN DYNAMICS , 2006 .

[41]  J. Brady,et al.  Dynamic simulation of hydrodynamically interacting suspensions , 1988, Journal of Fluid Mechanics.

[42]  Sriram Ramaswamy,et al.  Rheology of active-particle suspensions. , 2003, Physical review letters.

[43]  Peter A. Dewey,et al.  Propulsive performance of unsteady tandem hydrofoils in a side-by-side configuration , 2014 .

[44]  D. Weihs The hydrodynamics of dolphin drafting , 2004, Journal of biology.

[45]  P. F. Major,et al.  Predator-prey interactions in two schooling fishes, Caranx ignobilis and Stolephorus purpureus , 1978, Animal Behaviour.

[46]  Babak Hejazialhosseini,et al.  Reinforcement Learning and Wavelet Adapted Vortex Methods for Simulations of Self-propelled Swimmers , 2014, SIAM J. Sci. Comput..

[47]  H. A. Baldwin,et al.  Methods for measuring the three-dimensional structure of fish schools. , 1965, Animal behaviour.

[48]  Ole Arve Misund,et al.  Mapping the shape, size, and density of fish schools by echo integration and a high-resolution sonar , 1995 .

[49]  Petros Koumoutsakos,et al.  A Stochastic Model for Microtubule Motors Describes the In Vivo Cytoplasmic Transport of Human Adenovirus , 2009, PLoS Comput. Biol..

[50]  G. Taylor Analysis of the swimming of long and narrow animals , 1952, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[51]  A. Huth,et al.  The simulation of the movement of fish schools , 1992 .

[52]  D. Weihs Hydromechanics of Fish Schooling , 1973, Nature.

[53]  H. Chaté,et al.  Modeling collective motion: variations on the Vicsek model , 2008 .

[54]  Vicsek,et al.  Novel type of phase transition in a system of self-driven particles. , 1995, Physical review letters.

[55]  Triantafyllou,et al.  Near-body flow dynamics in swimming fish , 1999, The Journal of experimental biology.

[56]  Petros Koumoutsakos,et al.  Shape Optimization for Drag Reduction in Linked Bodies using Evolution Strategies and the Hybrid Wavelet Collocation - Brinkman Penalization Method , 2010 .

[57]  Eva Kanso,et al.  Dipole Interactions in Doubly Periodic Domains , 2013, J. Nonlinear Sci..

[58]  Steven V. Viscido,et al.  The effect of population size and number of influential neighbors on the emergent properties of fish schools , 2005 .

[59]  T. Pitcher,et al.  Fish in larger shoals find food faster , 1982, Behavioral Ecology and Sociobiology.

[60]  E. Kanso,et al.  Passive locomotion via normal-mode coupling in a submerged spring–mass system , 2009, Journal of Fluid Mechanics.

[61]  Eva Kanso,et al.  The finite-dipole dynamical system , 2012, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[62]  P. Saffman,et al.  The self-propulsion of a deformable body in a perfect fluid , 1967, Journal of Fluid Mechanics.

[63]  B L Partridge,et al.  The structure and function of fish schools. , 1982, Scientific American.

[64]  Hajime Tanaka,et al.  Purely hydrodynamic ordering of rotating disks at a finite Reynolds number , 2015, Nature Communications.

[65]  Darren Crowdy,et al.  Fluid-structure interaction of two bodies in an inviscid fluid , 2010 .