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Cellular Automata Modelling of Traffic in Human and Biological Systems

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Title: Cellular Automata Modelling of Traffic in Human and Biological Systems


1
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
2
Introduction
  • Modelling of transport problems
  • space, time, states can be discrete or continuous
  • various model classes

3
Overview
  • Highway traffic
  • Traffic on ant trails
  • Pedestrian dynamics
  • Intracellular transport
  • Unified description!?!

4
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

5
Asymmetric Simple Exclusion Process
6
Asymmetric Simple Exclusion Process
Caricature of traffic
  • Asymmetric Simple Exclusion Process (ASEP)
  • directed motion
  • exclusion (1 particle per site)

For applications different modifications
necessary
7
Influence of Boundary Conditions
  • open boundaries

Applications Protein synthesis
Surface growth
Boundary induced phase transitions
exactly solvable!
8
Phase Diagram
Maximal current phase JJ(p)
Low-density phase JJ(p,?)
High-density phase JJ(p,?)
9
Highway Traffic
10
Cellular Automata Models
  • Discrete in
  • Space
  • Time
  • State variables (velocity)

velocity
11
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)
12
Example
Configuration at time t Acceleration (vmax
2) Braking Randomization (p 1/3) Motion
(state at time t1)
13
Interpretation of the Rules
  • Acceleration Drivers want to move as fast as
    possible (or allowed)
  • Braking no accidents
  • Randomization
  • a) overreactions at braking
  • b) delayed acceleration
  • c) psychological effects (fluctuations in
    driving)
  • d) road conditions
  • 4) Driving Motion of cars

14
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

15
Fundamental Diagram
Relation current (flow) density
16
Metastable States
  • Empirical results Existence of
  • metastable high-flow states
  • hysteresis

17
VDR Model
  • Modified NaSch model
  • VDR model
    (velocity-dependent randomization)
  • Step 0 determine randomization pp(v(t))
  • p0 if v 0
  • p(v) with
    p0 gt p
  • p if v gt 0
  • Slow-to-start rule

18
Simulation of VDR Model
NaSch model
VDR model
VDR-model phase separation Jam stabilized by
Jout lt Jmax
19
Dynamics on Ant Trails
20
Ant trails
ants build road networks trail system
21
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.

22
Ant trail model
  1. motion of ants
  2. pheromone update (creation evaporation)

Dynamics
q
q
Q
f f f
parameters q lt Q, f
23
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
24
Spatio-temporal organization
  • formation of loose clusters

early times
steady state
coarsening dynamics
25
Pedestrian Dynamics
26
Collective Effects
  • jamming/clogging at exits
  • lane formation
  • flow oscillations at bottlenecks
  • structures in intersecting flows ( D.
    Helbing)

27
Pedestrian Dynamics
  • More complex than highway traffic
  • motion is 2-dimensional
  • counterflow
  • interaction longer-ranged (not only nearest
    neighbours)

28
Pedestrian model
idea Virtual chemotaxis chemical trace
long-ranged interactions are translated into
local interactions with memory
  • Modifications of ant trail model necessary since
  • motion 2-dimensional
  • diffusion of pheromones
  • strength of trace

29
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
30
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

31
Transition Probabilities
  • Total transition probability pij in direction
    (i,j)
  • pij N Mij exp(kDDij)
    exp(kSSij)(1-nij)
  • Mij matrix of preferences (preferred
    direction)
  • Dij dynamic floor field
    (interaction between pedestrians)
  • Sij static floor field
    (interaction with geometry)
  • kD, kS coupling strength
  • N normalization (? pij 1)

32
Lane Formation
velocity profile
33
Intracellular Transport
34
Intracellular Transport
  • Transport in cells
  • microtubule highway
  • molecular motor (proteins) trucks
  • ATP fuel

35
Kinesin and Dynein Cytoskeletal motors
Fuel ATP
ATP ADP P
Kinesin
Dynein
  • Several motors running on same track
    simultaneously
  • Size of the cargo gtgt Size of the motor
  • Collective spatio-temporal organization ?

36
Practical importance in bio-medical research
Disease Motor/Track Symptom
Charcot-Marie tooth disease KIF1B kinesin Neurological disease sensory loss
Retinitis pigmentosa KIF3A kinesin Blindness
Ushers syndrome Myosin VII Hearing loss
Griscelli disease Myosin V Pigmentation defect
Primary ciliary diskenesia/ Kartageners syndrome Dynein Sinus and Lung disease, male infertility
Goldstein, Aridor, Hannan, Hirokawa,
Takemura,.
37
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)
38
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)
39
Summary
  • Various very different transport and traffic
    problems can be described by similar models
  • 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

40
Collaborators
Thanx to
  • Duisburg
  • Michael Schreckenberg
  • Robert Barlovic
  • Wolfgang Knospe
  • Hubert Klüpfel

Rest of the World Debashish Chowdhury
(Kanpur) Ambarish Kunwar (Kanpur) Katsuhiro
Nishinari (Tokyo) T. Okada (Tokyo)
  • Cologne
  • Ludger Santen
  • Alireza Namazi
  • Alexander John
  • Philip Greulich

many others
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