massimo franceschetti university of california at berkeley

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MASSIMO FRANCESCHETTI University of California at Berkeley Phase transitions an engineering perspective

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Phase transitions an engineering perspective. MASSIMO FRANCESCHETTI University of California at Berkeley. Phase transition effect. when small changes in certain parameters of a system result in dramatic shifts in some globally observed behavior of the system. Example. - PowerPoint PPT Presentation

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MASSIMO FRANCESCHETTIUniversity of California at Berkeley

Phase transitions an engineering perspective

when small changes in certain parameters of a system result in dramatic shifts in some globally observed behavior of the system.

Phase transition effect

Examplepercolation theory, Broadbent and Hammersley (1957)

Example

cp Broadbent and Hammersley (1957)

2

1cp H. Kesten (1980)

pc0 p

P1

Gilbert (1961)

Mathematics Physics

Percolation theoryRandom graphs

Random Coverage ProcessesContinuum Percolation

Models of the internetImpurity ConductionFerromagnetism…

Universality, Ken Wilson Nobel prize

Grimmett (1989)Bollobas (1985)

Hall (1985)Meester and Roy (1996)

Broadbent and Hammersley (1957) Erdös and Rényi (1959)

Phase transitions in random graphs

Large scale networks of embedded devices

• Ad-Hoc networks• Sensor networks

Where are the phase transitions?

Uniform random distribution of points of density λ

One disc per pointStudies the formation of an unbounded connected component

First modelContinuum percolation, Gilbert (1961)

First modelContinuum percolation, Gilbert (1961)

The first paper in ad hoc wireless networks !

A

B

0.3 0.4

c0.35910…[Quintanilla, Torquato, Ziff, J. Physics A, 2000]

Example

N Unit area

Penrose (1997) Penrose Pisztora (1996)

Xue Kumar (2003)

Gilbert (1961) [Meester, Roy book (1996)]

Haggstrom Meester (1996)

Dousse Baccelli Thiran (2003)

Booth, Bruck, Franceschetti, Meester (2003)

2Density of points in

N

nNr

)(log~2

Nr

1~2

Nneighborsnearest log~

Continuum Percolation

Nearest neighbors percolation

Percolation with interference

Clustered networks

More wireless models

Towards a less idealistic modelFranceschetti, Booth, Cook, Meester, Bruck (2003)

Prob(correct reception)

Experiment

1

Connectionprobability

d

Continuum percolationContinuum percolation

2r

Our modelOur model

d

1

Connectionprobability

Connectivity model

Connectionprobability

1

x

A first order question

How does the percolation threshold cchange?

Squishing and Squashing

Connectionprobability

x

) ()( xpgpxgs

)(xg

2

)())((x

xgxgENC

))(())(( xgsENCxgENC

2

)(0x

xg

Theorem

))(())(( xgsxg cc

For all

“longer links are trading off for the unreliability of the connection”

“it is easier to reach connectivity in an unreliable network”

Shifting and Squeezing

Connectionprobability

x

)(

0

1

)()(

))(()(yhs

s

y

dxxxgxdxxgss

xhgxgss

)(xg

2

)())((x

xgxgENC

))(())(( xgssENCxgENC

)(xgss

Example

Connectionprobability

x

1

Mixture of short and long edges

Edges are made all longer

Do long edges help percolation?

2

)(0x

xg

Conjecture

))(())(( xgssxg cc

For all

Theorem

For all , there exists a finite , such that gss r*(x) percolates, for all )(1 * gc rr * *

It is possible to decrease the percolation threshold by taking a sufficiently large shift !

For all 2

)(0x

xg

CNP

Squishing and squashing Shifting and squeezing

What have we proven?

(sporadic) long links help the percolation process

CNP

Among all convex shapes the hardest to percolate is centrally symmetricJonasson (2001)

Is the disc the hardest shape to percolate overall?

What about non-circular shapes?

CNP

To the engineer: above 4.51 we are fine!To the theoretician: can we prove “disc is hardest” conjecture?

can we exploit long links for routing?

Bottom line

Small World Networks

Regular RandomSmall World

Watts Strogatz (1998)

Kleinberg (2000) Franceschetti & Meester (2003)

Routing in a small world

• Nodes on the grid• Fixed number of contacts• Probability scales with distance

• Nodes on the plane• Random number contacts in a given region • Density scales with distance

each node has only local information of the network connectivity

Routing in a small world

Connections of z are PPP of density

-delivery occurs when msg is delivered within to target

S

T

Routing in a small world

S

T

d

Routing in a small world

S

T

d

Scale the number of neighbors as 1/x2 to obtain efficient routing

Not only graphs…

One application

A pursuit evasion gameSinopoli, Schenato, Franceschetti, Poolla, Sastry (2003)

A pursuit evasion game

A pursuit evasion game

A pursuit evasion game

A pursuit evasion game

A pursuit evasion game

A pursuit evasion game

A pursuit evasion game

A pursuit evasion game

A pursuit evasion game

A pursuit evasion game

A pursuit evasion game

A pursuit evasion game

• Goal: given observations find the best estimate (minimum variance) for the state

• But may not arrive at each time step when traveling over a sensor network

Intermittent observations

Problem formulation

System

Kalman Filter

M

z-1

ut

et

xt

M

z-1

K+

+

+

-

xt+1

yt+1

• Discrete time LTI system

• and are Gaussian random variables with zero mean and covariance matrices Q and R positive definite.

Loss of observation

• Discrete time LTI system

Let it have a “huge variance” when the observation does not arrive

Loss of observation

• The arrival of the observation at time t is a binary random variable

• Redefine the noise as:

Kalman Filter with losses

Derive Kalman equations using a “dummy” observation when

then take the limit for t=0

Results on mean error covariance Pt

ci

cPt

ctt

PtMPE

PPE

||max

11

0condition initialany and 1for ][

0condition initial some and 0for ][lim

0

0

0

Special cases

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 10

10

20

30

40

50

60

70

80

90

100S

,

V

c

C is invertible, or A has a single unstable eigenvalue

Conclusion• Phase transitions are a fundamental effect in

engineering systems with randomness• There is plenty of formal work to be done

For papers:

[email protected]

“Navigation in small world networks, a continuum scale-free model”Franceschetti and Meester

Preprint ‘03

“Percolation in wireless multi-hop networks”, Franceschetti, Booth, Cook, Meester, Bruck

ISIT ’03 and Submitted to IEEE Trans. Info Theory

“Covering algorithm continuum percolation and the geometry of wireless networks”Booth, Bruck, Franceschetti, Meester

Annals of Applied Probability, 13(2), May 2003.

“Kalman Filtering with intermittent observations”Sinopoli, Schenato, Franceschetti, Poolla, Sastry

CDC ’03 and Submitted to IEEE Trans. Automatic Control