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Cellular Automata Modelling of Traffic in Human and Biological Systems. Andreas Schadschneider Institute for Theoretical Physics University of Cologne. www.thp.uni-koeln.de/~as. www.thp.uni-koeln.de/ant-traffic. Introduction. Modelling of transport problems:
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Cellular Automata Modelling of Traffic in Human and Biological Systems Andreas Schadschneider Institute for Theoretical Physics University of Cologne www.thp.uni-koeln.de/~as www.thp.uni-koeln.de/ant-traffic
Introduction • Modelling of transport problems: • space, time, states can be discrete or continuous • various model classes
Overview • Highway traffic • Traffic on ant trails • Pedestrian dynamics • Intracellular transport • Unified description!?!
Cellular Automata Cellular automata (CA) are discrete in space time state variable (e.g. occupancy, velocity) Advantage: very efficient implementation for large-scale computer simulations often: stochastic dynamics
Asymmetric Simple Exclusion Process q q • Asymmetric Simple Exclusion Process (ASEP): • directed motion • exclusion (1 particle per site) Caricature of traffic: For applications: different modifications necessary
Highway Traffic
Cellular Automata Models • Discrete in • Space • Time • State variables (velocity) velocity
Update Rules • Rules (Nagel-Schreckenberg 1992) • Acceleration: vj! min (vj + 1, vmax) • Braking: vj! min ( vj , dj) • Randomization: vj ! vj – 1 (with probability p) • Motion: xj! xj + vj (dj = # empty cells in front of car j)
Example Configuration at time t: Acceleration (vmax = 2): Braking: Randomization (p = 1/3): Motion (state at time t+1):
Simulation of NaSch Model • Reproduces structure of traffic on highways • - Fundamental diagram • - Spontaneous jam formation • Minimal model: all 4 rules are needed • Order of rules important • Simple as traffic model, but rather complex as stochastic model
Fundamental Diagram Relation: current (flow) $ density
Metastable States • Empirical results: Existence of • metastable high-flow states • hysteresis
VDR Model • Modified NaSch model: • VDR model (velocity-dependent randomization) • Step 0: determine randomization p=p(v(t)) • p0 if v = 0 • p(v) = with p0 > p • p if v > 0 • Slow-to-start rule
Simulation of VDR Model NaSch model VDR model VDR-model: phase separation Jam stabilized by Jout < Jmax
Dynamics on Ant Trails
Ant trails ants build “road” networks: trail system
Chemotaxis • Ants can communicate on a chemical basis: • chemotaxis • Ants create a chemical trace of pheromones • trace can be “smelled” by other • ants follow trace to food source etc.
Ant trail model qqQ • motion of ants • pheromone update (creation + evaporation) Dynamics: q q Q f f f parameters: q < Q, f
Fundamental diagram of ant trails velocity vs. density non-monotonicity at small evaporation rates!! Experiments: Burd et al. (2002, 2005) different from highway traffic: no egoism
Spatio-temporal organization • formation of “loose clusters” early times steady state coarsening dynamics
Pedestrian Dynamics
Collective Effects • jamming/clogging at exits • lane formation • flow oscillations at bottlenecks • structures in intersecting flows ( D. Helbing)
Pedestrian Dynamics • More complex than highway traffic • motion is 2-dimensional • counterflow • interaction “longer-ranged” (not only nearest neighbours)
Pedestrian model idea: Virtual chemotaxis chemical trace: long-rangedinteractions are translated intolocalinteractions with ‘‘memory“ • Modifications of ant trail model necessary since • motion 2-dimensional: • diffusion of pheromones • strength of trace
Floor field cellular automaton • Floor field CA: stochastic model, defined by transition probabilities, only local interactions • reproduces known collective effects (e.g. lane formation) Interaction: virtual chemotaxis (not measurable!) dynamic + static floor fields interaction with pedestrians and infrastructure
Transition Probabilities • Stochastic motion, defined by • transition probabilities • 3 contributions: • Desired direction of motion • Reaction to motion of other pedestrians • Reaction to geometry (walls, exits etc.) • Unified description of these 3 components
Lane Formation velocity profile
Intracellular Transport
Intracellular Transport • Transport in cells: • microtubule = highway • molecular motor (proteins) = trucks • ATP = fuel
Kinesin and Dynein: Cytoskeletal motors Fuel: ATP ATP ADP + P Kinesin Dynein • Several motors running on same track simultaneously • Size of the cargo >> Size of the motor • Collective spatio-temporal organization ?
Practical importance in bio-medical research Goldstein, Aridor, Hannan, Hirokawa, Takemura,…………….
ASEP-like Model of Molecular Motor-Traffic ASEP + Langmuir-like adsorption-desorption Parmeggiani, Franosch and Frey, Phys. Rev. Lett. 90, 086601 (2003) D A q a b Also, Evans, Juhasz and Santen, Phys. Rev.E. 68, 026117 (2003)
Spatial organization of KIF1A motors: experiment MT (Green) 10 pM KIF1A (Red) 100 pM 1000pM 2 mM of ATP 2 mm position of domain wall can be measured as a function of controllable parameters. Nishinari, Okada, Schadschneider, Chowdhury, Phys. Rev. Lett. (2005)
Summary • Various very differenttransport and traffic problems can be described by similarmodels • Variants of the Asymmetric Simple Exclusion Process • Highway traffic: larger velocities • Ant trails: state-dependent hopping rates • Pedestrian dynamics: 2d motion, virtual chemotaxis • Intracellular transport: adsorption + desorption
Collaborators Cologne: Ludger Santen Alireza Namazi Alexander John Philip Greulich Duisburg: Michael Schreckenberg Robert Barlovic Wolfgang Knospe Hubert Klüpfel Thanx to: Rest of the World: Debashish Chowdhury (Kanpur) Ambarish Kunwar (Kanpur) Katsuhiro Nishinari (Tokyo) T. Okada (Tokyo) + many others