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Zelf Organiserende Systemen ZOS

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Title: Zelf Organiserende Systemen ZOS


1
Zelf Organiserende Systemen (ZOS) - Self
Organising Systems - Vrij Universiteit
Amsterdam Lecture 5 Self Organisation to
Criticality http//www.cs.vu.nl/zos Martijn
Schut schut_at_cs.vu.nl
2
SOS - Lecture 5
Overview
  • Criticality in theory
  • Sandpiles
  • and in practice
  • Forest fires
  • Ecosystems (Lotka-Volterra)
  • Panic
  • Chaos
  • Exercises
  • Turing Machines
  • This week
  • Panic

3
SOS - Lecture 5
Criticality
  • What came first, chicken or egg?
  • Biological systems are organised by the
    information present in them, and the information
    in turn originates in the sel-organised state by
    means of selection. (Adami, 1998)
  • self-organisation is one of the hallmarks of
    living systems
  • selection relates criticality to evolution (week
    7)

4
SOS - Lecture 5
Critical Values
5
SOS - Lecture 5
Criticality
  • Some important things to remember
  • self organised means that critical values are
    included with the system
  • in chaotic systems, critical values can make the
    system abdruptly change state
  • These two characteristics are illustrated in
    this Lectures examples

6
SOS - Lecture 5
Sandpiles
  • What is the problem?
  • Very simple
  • Imagine a chess board with miniscule squares.
    Let grains of sand drop on this board at random
    locations for an extended amount of time.
  • What do you see?
  • Many events where only one grain topples
  • Some events where a few grains are involved in
    an avalanche
  • Rare events where all grains are involved in an
    avalanche
  • We are interested to know what the distribution
    is of these size of events

7
SOS - Lecture 5
Sandpiles
  • Solution?
  • Surprisingly difficult to analyse from first
    principles!
  • Quite easy to see by simple performing the
    experiment
  • Experiments result in very nice graphs
  • Can we use these experiments for analysis?

8
SOS - Lecture 5
Sandpiles
A one-dimensional sandpile
9
SOS - Lecture 5
Sandpiles
  • Rules
  • if difference in sizes between locations is gt
    2, then one grain will tumble to the next
    location
  • Even in this extremely simple example, it is very
    hard to
  • predict the size of avalanches over time.

10
SOS - Lecture 5
Sandpiles
But what turns out to be the case? With
experiments, we find that there is one critical
state towhich the system always returns! /
Note state is defined on the average slope /
11
SOS - Lecture 5
Sandpiles
  • What does such a state look like?
  • Assume building up from an empty row to a state
    just beforea sliding event (avalanche
    involving all locations)
  • In this state, the first location is always
    maximally filled and the differences between
    locations is critical

12
SOS - Lecture 5
Sandpiles
  • Take home message
  • critical state itself is very unstable
  • but it makes the whole system very stable

13
SOS - Lecture 5
Forest Fires
Example State
  • Example Rules
  • B ? A
  • A ? T
  • BT ? AB
  • T ? B
  • B ? A
  • Legend
  • T Tree
  • B Burning
  • A Ashes

14
SOS - Lecture 5
Forest Fires
  • With these states and rules, the system is not
    critical!
  • Instead it is periodic, like disease epidemics
  • Over time there will be waves of live and dead
    trees
  • What to do to make it critical, what is the
    problem here?
  • The system is not driven!
  • A driving force is an infinitely small external
    cause of fluctuation
  • Thus there is nothing to make it revert to a
    single state

15
SOS - Lecture 5
Forest Fires
  • Solution light up a cigarette!
  • Or have an occasional lightning strike
  • This changes the system into a critical one
  • Now trees start burning spontaneously
  • Thus T ? B with some very small probability
  • The critical state is then one in which there is
    some constantnumber of burning trees

16
SOS - Lecture 5
Properties of self criticality
  • The system must
  • resemble or be a self organising system, I.e.
    many interactingsmall components
  • carry information throughout the whole system
  • carry noise (random elements) throughout the
    whole system
  • an infinitesimal driving rate

17
SOS - Lecture 5
Chaos Theory
  • This driving rate reminds a bit of chaos theory
  • Are chaotic systems and critical systems related?

18
SOS - Lecture 5
Chaos Theory
  • Chaos happens in dynamic systems
  • These are basically systems in which the
    components are in motion
  • Order in such a system occurs when it is in
    balance
  • In balance means
  • little disturbances have no consequences
  • action reaction
  • only dramatic disturbances can cause state
    transactions

19
SOS - Lecture 5
Chaos Theory
Examples of systems in balance
ice
sand
20
SOS - Lecture 5
Chaos Theory
21
SOS - Lecture 5
Chaos Theory
  • Lorenz Curve
  • Discovered by Lorenz in 60s
  • Meteorologist
  • How predictable is the weather?

22
SOS - Lecture 5
Chaos Theory
23
SOS - Lecture 5
Chaos Theory
  • Is this not very exceptional?
  • No, we can see chaos in
  • turbulence of water and air
  • wobbling of the planets
  • global weather patterns
  • electric-chemical activity in the human brain

24
SOS - Lecture 5
Chaos Theory
  • Then how is it different from stochastics?
  • It is exactly the opposite!
  • With probabilities, we are able to predict
    long-term outcomes
  • For example, flipping a coin
  • (remember the law of large numbers?)

25
SOS - Lecture 5
Ecologies
An ecosystem is also a self organising critical
system withemerging properties, interacting
components etc etc...
26
SOS - Lecture 5
Ecologies
27
SOS - Lecture 5
Ecologies
Click here for to see some major state shifts and
their causes
28
SOS - Lecture 5
Patchiness
29
SOS - Lecture 5
Patchiness
30
SOS - Lecture 5
Patchiness
double nextValue(int i, int j) double
nextValue double neighbourhood new
doublenbhWidthnbhLength neighbourhood
makeNbh(i, j) double nbhValue
computeNbhValue(neighbourhood) nextValue
worldij Math.max(B, Math.min(H,
cnbhValue)) return nextValue
double computeNbhValue(double nbh)
double nbhValue 0 int k, l for(k0
kltnbhWidth k) for(l0 lltnbhLength
l) if(!(knbhCenterX l nbhCenterY))
nbhValue nbhklcMatrixkl
return nbhValue
31
SOS - Lecture 5
Patchiness
32
SOS - Lecture 5
Panic
  • Panic behaviour is also self organising
  • Trade off between well being of the individual
    and the group
  • People never make this choice rationally
  • People have investigated panic theoretically
    with experiments
  • Use the results of these experiments to guide
    people in panic situations

33
SOS - Lecture 5
Panic - Example Simulations
no panic panic stampede fire front column straigh
t corridor corridor with widening herding individ
ualism mixed behaviour
34
SOS - Lecture 5
Panic - 2 exits
  • People are searching for an exit they can't see
    because of smoke (grey), the desired velocity of
    individuals is v0 5 m/s.
  • Pedestrians recognize the door and the walls
    from a distance of 2m, while the range of
    pedestrian-pedestrian interactions is assumed to
    be 5m.
  • For pure individualism (unrealistic), people
    find an exit only by chance.
  • For strong herding, people follow the mass which
    may move into the wrong direction.
  • Most efficient is a mixture of individualism and
    herding, for which small groups are formed
    Successful strategies that individuals found by
    chance are imitated by a reasonable number of
    people.

35
SOS - Lecture 5
Panic - Simulation - 2 exits
Type of Behaviour Escaped until t
20s Individualism (p0.01) 66 Mixed behavior
(p0.4) 71 Herding (p0.8) 16
36
SOS - Lecture 5
Conclusions
  • Criticality in theory
  • Sandpiles
  • and in practice
  • Forest fires
  • Ecosystems (Lotka-Volterra)
  • Panic
  • Chaos
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