Crowd Control: A physicist’s approach to collective human behaviour
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Transcript of Crowd Control: A physicist’s approach to collective human behaviour
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Crowd Control:A physicist’s approach to collective
human behaviour
T. Vicsek
Principal collaborators:
A.L. Barabási, A. Czirók, I. Farkas, Z. Néda and D. Helbing
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Group motion of people: lane formation
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Ordered motion (Kaba stone, Mecca)
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Collective “action”: Mexican wave
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STATISTICAL PHYSICS OF COLLECTIVE BEHAVIOUR
Collective behaviour is a typical feature of living systems consisting of many similar units
Main feature of collective phenomena: the behaviour of the units becomes similar, but very different from what they would exhibit in the absence of the others
Main types: (phase) transitions, pattern/network formation,
synchronization*, group motion*
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- Methods of statistical physics can be successfully used to interpret collective behaviour
- The above mentioned behavioural patterns can be observed and quantitatively described/explained for a wide range of phenomena starting from the simplest manifestations of life (bacteria) up to humans because of the principle of universality
• CONCEPT
•Experimentally observed simple behaviour of a very complex system (people) is interpreted with models taking into account details of “reality”.
•See, e.g.: Fluctuations and Scaling in Biology, T. Vicsek, ed. (Oxford Univ. Press, 2001)
MESSAGE
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bacteria
robots
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Synchronization
Dependence of sound intensityOn time
• Examples: (fire flies, cicada, heart, steps, dancing, etc) • “Iron” clapping: collective human behaviour allowing quantitative analysis
Nature, 403 (2000) 849
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Time
Frequency
Fourier-gram of rhythmic applause
Darkness is proportional to the magnitude of the power spectrum
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Mexican wave (La Ola)
Phenomenon :
• A human wave moving along the stands of a stadium
• One section of spectators stands up, arms lifting, then sits down as the next section does the same.
Interpretation: using modified models originally proposed for excitable media such as heart tissue or amoeba colonies
Nature, 419 (2002) 131
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Mexican wave
Typical
Speed: 12 m/sec
width: 10 m/sec
direction: clockwise
Appears usually
during less exciting
periods of the game
Nature, 419 (2002) 131
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Model: excitable medium Excitable: inactive can be activated (I>c!)
active : active cannot be activated
refractory: inactive cannot be activated
Examples:
* fire fronts
* cardiac tissue
* Belousov-
Zabotinsky re-
action
* aggregation of
amoebae
Three states
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Simulation – demoone inactive and 5 five active/refractory stages
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Results
Number of initiators
threshold
Probability of generating a wave
This approach has the potential of interpreting the spreading of excitement in crowds under more complex conditions
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Group motion of humans (theory)
Model:
- Newton’s equations of motion
- Forces are of social, psychological or physical origin
(herding, avoidance, friction, etc)
Statement:
- Realistic models useful for interpretation of
practical situations and applications can be
constructed
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2d
1dt
t+tt+2t
-------------------------------------------------------------------------------------------------
Simplest aspect of group motion: flocking, herding
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Swarms, flocks and herds
• Model: The particles - maintain a given velocity - follow their neighbours - motion is perturbed by fluctuations
• Result: ordering is
due to motion
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What is displayed in this experimental picture?
Directions of prehairs on the wing of a mutant fruitfly(the gene responsible for global directionality is kicked out, wihle the one enforcing local alignment is operational)
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Group motion of humans (observations)
Pedestrian crossing: Self-
organized lanes
Corridor in stadium: jamming
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Escaping from a narrow corridor
Large perturbatons Smaller perturbations
The chance of escaping (ordered motion) depends on the level of “excitement” (on the level of perturbations relative to the “follow the others” rule)
Phys. Rev. Lett. (1999)
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EQUATION OF MOTION for the velocity of pedestrian i
, exp
, )()()( 00
ijtjiijijijijijiijijiij
iWij
iji
iiii
ii
tvdrgndrkgBdrAf
fftvtetv
mdt
dvm
“psychological / social”, elastic repulsion and sliding friction force terms, and g(x) is zero, if dij > rij , otherwise it is equal to x.
MASS BEHAVIOUR: herding
, )(1 )( 00
jjiiii tepepNte
. ofion normalizat denotes )( where zzzzN
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Social force:”Crystallization” in a pool
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Moving along a wider corridor
Typical situation crowd
• Spontaneous segregation (build up of lanes)• optimization
Phys. Rev. Lett. (2000)
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Panic
• Escaping from a closed area through a door• At the exit physical forces are dominant !
Nature, 407 (2000) 487
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Paradoxial effects
•obstacle: helps (decreases the presure)•widening: harms (results in a jamming-like effect)
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“Panic at the rock concert in Brussels”
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Effects of herding
• Dark room with two exits• Changing the level of herding
medium
No herding
Total herding
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http://angel.elte.hu/~vicsek
http://angel.elte.hu/wave
http://angel.elte.hu/panic
http://www.nd.edu/~networks/clap
Mexican wave
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Collective motion
Patterns of motion of similar, interacting organisms
Humans
Cells Flocks, herds, etc
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A simple model: Follow your neighbors !
)()(
)()1( 0 t
tv
tvvtv j
Ri
Rij
•absolute value of the velocity is equal to v0
• new direction is an average of the directions of
neighbors
• plus some perturbation ηj(t)
•Simple to implement
• analogy with ferromagnets, differences:
for v0 << 1 Heisenberg-model like behavior
for v0 >> 1 mean-field like behavior
in between: new dynamic critical phenomena (ordering, grouping, rotation,..)
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Acknowledgements
Principal collaborators:
Barabási L., Czirók A., Derényi I., Farkas I., Farkas Z.,Hegedűs B., D. Helbing, Néda Z., Tegzes P.
Grants from: OTKA, MKM FKFP/SZPÖ, MTA, NSF
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Social force:”Crystallization” in a pool
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Major manifestations
Pattern/network formation :
• Patterns: Stripes, morphologies, fractals, etc
• Networks: Food chains, protein/gene interactions, social connections, etc
Synchronization: adaptation of a common phase during periodic behavior
Collective motion:
• phase transition from disordered to ordered
• applications: swarming (cells, organisms),
segregation, panic
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Motion driven by fluctuations
Molecular motors:Protein molecules moving in a strongly fluctuatig environment along chains of complementary proteins
Our model:Kinesin moving along microtubules (transporting cellular organelles).
„scissors” like motion in a periodic, sawtooth shaped potential
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Transport of a polymer through a narrow holeMotivation: related experiment, gene therapy, viral infectionModel: real time dynamics (forces, time scales, three dimens.)
Translocation of DNS through a nuclear pore
duration: 1 msLengt of DNS: 500 nm
duration: 12 sLength of DNS : 10 m
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Collective motion
Humans
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Ordered motion (Kaba stone, Mecca)