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Transportation Science and the Dynamics of Critical Infrastructure Networks Anna Nagurney John F. Smith Memorial Professor Isenberg School of Management University of Massachusetts - Amherst Civil and Environmental Engineering Seminar December 7, 2006

Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

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Page 1: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Transportation Science and theDynamics of

Critical Infrastructure Networks

Anna NagurneyJohn F. Smith Memorial ProfessorIsenberg School of Management

University of Massachusetts - Amherst

Civil and Environmental Engineering SeminarDecember 7, 2006

Page 2: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Funding for our research has been provided by:

National Science Foundation

AT&T Foundation

John F. Smith Memorial Fund -University of Massachusetts atAmherst

Page 3: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Outline of Presentation:

• Background• Brief History of the Science of Networks• Interdisciplinary Impact of Networks• The Braess Paradox• Methodological Tools• Some Interesting Critical Infrastructure Networks• The Time-Dependent (Demand-Varying) Braess Paradox• A New Network Performance/Efficiency Measure with

Applications to Critical Infrastructure Networks• New Challenges and Opportunities: Unification of Evolutionary

Variational Inequalities and Projected Dynamical Systems

Page 4: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Components of Common PhysicalNetworks

Network System Nodes Links Flows

Transportation Intersections,Homes,Workplaces,Airports,Railyards

Roads,Airline Routes,Railroad Track

Automobiles,Trains, andPlanes,

Manufacturingand logistics

Workstations,DistributionPoints

Processing,Shipment

Components,Finished Goods

Communication Computers,Satellites,TelephoneExchanges

Fiber OpticCablesRadio Links

Voice,Data,Video

Energy PumpingStations,Plants

Pipelines,TransmissionLines

Water,Gas, Oil,Electricity

Page 5: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

US Railroad Freight Flows

Page 6: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Internet Traffic Flows Over One 2Hour Period

from Stephen Eick, Visual Insights

Page 7: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Electricity is Modernity

Page 8: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The scientific study of networksinvolves:

• how to model such applications asmathematical entities,

• how to study the models qualitatively,

• how to design algorithms to solve theresulting models.

Page 9: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The basic components ofnetworks are:

• Nodes

• Links or arcs

• Flows

Page 10: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Nodes Links Flows

12 13 14 15

7 9

3

16

4

1817 19 20

8

1 2

6

5

10

11

Page 11: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Brief History of the Science of Networks

1736 - Euler - the earliest paper on graph theory -Konigsberg bridges problem.

1758 - Quesnay in his Tableau Economiqueintroduced a graph to depict the circular flow offinancial funds in an economy.

Page 12: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

1781 - Monge, who had worked under NapoleonBonaparte, publishes what is probably the first paperon transportation in minimizing cost.

1838 - Cournot states that a competitive price isdetermined by the intersection of supply and demandcurves in the context of spatially separate markets inwhich transportation costs are included.

1841 - Kohl considered a two node, two routetransportation network problem.

1845 - Kirchhoff wrote Laws of Closed Electric Circuits.

Page 13: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

1920 - Pigou studied a transportation network system of tworoutes and noted that the decision-making behavior of theusers on the network would result in different flow patterns.

1936 - Konig published the first book on graph theory.

1939, 1941, 1947 - Kantorovich, Hitchcock, and Koopmansconsidered the network flow problem associated with theclassical minimum cost transportation problem and providedinsights into the special network structure of these problems,which yielded special-purpose algorithms.

1948, 1951 - Dantzig published the simplex method for linearprogramming and adapted it for the classical transportationproblem.

Page 14: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

1951 - Enke showed that spatial price equilibriumproblems can be solved using electronic circuits

1952 - Copeland in his book asked, Does money flowlike water or electricity?

1952 - Samuelson gave a rigorous mathematicalformulation of spatial price equilibrium andemphasized the network structure.

Page 15: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

1956 - Beckmann, McGuire, and Winsten in theirbook, Studies in the Economics of Transportation,provided a rigorous treatment of congested urbantransportation systems under different behavioralmechanisms due to Wardrop (1952).

1962 - Ford and Fulkerson publish Flows inNetworks.

1969 - Dafermos and Sparrow coined the terms user-optimization and system-optimization and developalgorithms for the computation of solutions thatexploit the network structure of transportationproblems.

Page 16: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

NetworksNetworks

management science/management science/operations researchoperations research

engineering/engineering/physicsphysics

appliedappliedmathematicsmathematics

computercomputersciencescience

publicpublicpolicypolicy biologybiology

economicseconomicsand financeand finance

Networks in Different Disciplines

Page 17: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Interdisciplinary Impactof Networks

Networks

Energy

Manufacturing

Telecommunications

Transportation

Interregional Trade

General Equilibrium

Industrial Organization

Portfolio Optimization

Flow of FundsAccounting

Engineering

Computer Science

Routing Algorithms

Economics

Biology

DNA Sequencing

Targeted CancerTherapy

Sociology

Social Networks

OrganizationalTheory

Page 18: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Characteristics of Networks Today

• large-scale nature and complexity of networktopology;

• congestion;• alternative behavior of users of the network, which

may lead to paradoxical phenomena;• the interactions among networks themselves such as

in transportation versus telecommunications;• policies surrounding networks today may have a

major impact not only economically but also socially,politically, and security-wise.

Page 19: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

• alternative behaviors of the users of thenetwork

– system-optimized versus

– user-optimized (network equilibrium),

which may lead to

paradoxical phenomena.

Page 20: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Transportation science has historically been thediscipline that has pushed the frontiers interms of methodological developments forsuch problems (which are often large-scale)beginning with the work of Beckmann,McGuire, and Winsten (1956).

Page 21: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The Braess (1968) ParadoxAssume a network with a singleO/D pair (1,4). There are 2paths available to travelers:p1=(a,c) and p2=(b,d).For a travel demand of 6, theequilibrium path flows are xp1

*

= xp2* = 3 and

The equilibrium path travel costisCp1

= Cp2= 83.

32

1

4

a

c

b

d

ca(fa)=10 fa cb(fb) = fb+50

cc(fc) = fc+50 cd(fd) = 10 fd

Page 22: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Adding a LinkIncreases Travel Cost for All!

Adding a new link creates a new pathp3=(a,e,d).The original flow distribution pattern isno longer an equilibrium pattern, sinceat this level of flow the cost on path p3,Cp3=70.The new equilibrium flow patternnetwork is xp1

* = xp2* = xp3

*=2.The equilibrium path travel costs: Cp1 =Cp2 = Cp3

= 92.

32

1

4

a

c

b

d

e

ce(fe) = fe + 10

Page 23: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The 1968 Braess article has been translated fromGerman to English and appears as

On a Paradox of Traffic Planning

by Braess, Nagurney, Wakolbinger

in the November 2005 issue of TransportationScience.

Page 24: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The tools that we are using in ourDynamic Network research include:

• network theory• optimization theory• game theory• variational inequality theory• evolutionary variational inequality theory• projected dynamical systems theory• double-layered dynamics theory• network visualization tools.

Page 25: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Dafermos (1980) showed that the transportationnetwork equilibrium (also referred to as user-optimization) conditions as formulated by Smith(1979) were a finite-dimensional variationalinequality.

In 1993, Dupuis and Nagurney proved that the set ofsolutions to a variational inequality problemcoincided with the set of solutions to a projecteddynamical system (PDS) in Rn.

In 1996, Nagurney and Zhang published ProjectedDynamical Systems and VariationalInequalities.

Page 26: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

VI Formulation of TransportationNetwork Equilibrium (Dafermos (1980),

Smith (1979))

Page 27: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

x0

A Geometric Interpretation of a Variational Inequalityand a

Projected Dynamical System (Dupuis and Nagurney(1993), Nagurney and Zhang (1996))

Page 28: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Some Interesting Applications

• Telecommuting/Commuting Decision-Making• Teleshopping/Shopping Decision-Making• Supply Chain Networks with Electronic Commerce• Financial Networks with Electronic Transactions• Reverse Supply Chains with E-Cycling• Knowledge Networks• Energy Networks/Power Grids• Social Networks integrated with Economic

Networks

Page 29: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Nagurney, Ke, Cruz, Hancock, Southworth, Environment and Planning B (2002)

Page 30: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The Electric Power Supply Chain Network

Nagurney and Matsypura, Proceedings of the CCCT (2004)

Page 31: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The Equivalence of Supply Chain Networksand Transportation Networks

Nagurney, Transportation Research E (2006)

Page 32: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Copeland (1952) wondered whether moneyflows like water or electricity.

Liu and Nagurney have shown that moneyand electricity flow like transportationnetwork flows (Computational ManagementScience (2006)).

Page 33: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The Transportation Network EquilibriumReformulation of the Financial NetworkEquilibrium Model with Intermediation

Page 34: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The fifth chapter of Beckmann, McGuire, and Winsten’sbook, Studies in the Economics of Transportation(1956) describes some unsolved problems includinga single commodity network equilibrium problem thatthe authors imply could be generalized to captureelectric power networks.

Page 35: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The Transportation Network EquilibriumReformulation of Electric Power Supply Chain

Networks

Electric Power Supply TransportationChain Network Network

Nagurney et al, to appear in Transportation Research E

Page 36: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

We have, hence, shown that money as well aselectricity flow like transportation and haveanswered questions posed fifty years ago byCopeland and Beckmann, McGuire, andWinsten, respectively.

Page 37: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

We are using evolutionary variational inequalities tomodel dynamic networks with:

• dynamic (time-dependent) supplies and demands

• dynamic (time-dependent) capacities

• structural changes in the networks themselves.

Such issues are important for robustness, resiliency,and reliability of networks (including supply chainsand the Internet).

Page 38: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

What happens if the demand is varied inthe Braess Network?

The answer lies in the solution of anEvolutionary (Time-Dependent)Variational Inequality.

Nagurney, Parkes, and Daniele, Computational Management Science (2006)

Page 39: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Recall the Braess Networkwhere we add the link e. 32

1

4

a

c

b

d

e

Page 40: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

0

5

10

0 10 20Demand(t) = t

Equi

libriu

m P

ath

Flow

Paths 1 and 2Path 3

I II III

The Solution of an Evolutionary (Time-Dependent) Variational Inequality

for the Braess Network with Added Link (Path)

3.64 8.88

Braess Network withTime-DependentDemands

Page 41: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

In Demand Regime I, only the new path is used.In Demand Regime II, the Addition of a New Link (Path) Makes EveryoneWorse Off!In Demand Regime III, only the original paths are used.

0

40

80

120

160

0 5 10 15 20

Demand

Cos

t of U

sed

Path

s

Network 1

Network 2

I II III

Network 1 is the Original Braess Network - Network 2 has the added link.

Page 42: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The new link is NEVER used after acertain demand is reached even if thedemand approaches infinity.

Hence, in general, except for a limitedrange of demand, building the new linkis a complete waste!

Page 43: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

• Recent disasters have demonstrated theimportance as well as the vulnerability ofcritical infrastructure networks.

• For example:– Hurricane Katrina, August 23, 2005– The biggest blackout in North America,

August 14, 2003– 9/11 Terrorist Attacks, September 11, 2001

Page 44: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

An Urgent Need for a NetworkEfficiency/Performance Measure

In order to be able to assess theperformance/efficiency of a network, it isimperative that appropriate measures be devised.

Appropriate network measures can assist in theidentification of the importance of networkcomponents, that is, nodes and links, and theirrankings. Such rankings can be very helpful in thecase of the determination of network vulnerabilitiesas well as when to reinforce/enhance security.

Page 45: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The Network Efficiency Measureof Latora and Marchiori (2001)

• Latora and Marchiori (2001) proposed anetwork efficiency measure (the L-Mmeasure) as follows:

Page 46: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The Network Efficiency Measureof Nagurney and Qiang (2006)

• Nagurney and Qiang (2006) proposed a networkefficiency measure (the N-Q measure) whichcaptures the demand and flow information underthe network equilibrium. It is defined as follows:

Page 47: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance of a Network Component

Page 48: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The Approach to Study the Importance ofNetwork Components

The elimination of a link is treated in the N-Qmeasure by removing that link while theremoval of a node is managed by removingthe links entering and exiting that node. In thecase that the removal results in no pathconnecting an O/D pair, we simply assign thedemand for that O/D pair to an abstract pathwith a cost of infinity.

Hence, our measure is well-defined even in thecase of disconnected networks.

Page 49: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

The L-M Measurevs.

the N-Q Measure

Page 50: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Application I: the Braess (1968) Network

Assume a network with a single O/Dpair (1,4). There are 2 pathsavailable to travelers: p1=(a,c) andp2=(b,d).For a travel demand of 6, theequilibrium path flows are xp1

*=xp2

*=3.The equilibrium path travel cost isCp1=Cp2=83.

1

2 3

4

a b

c d

ca(fa)=10fa cb(fb)= fb+50

cc(fc)=fc+50 cd(fd)= 10fd

Page 51: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Adding a Link Increases Travel Cost for All!

Adding a new link creates a new pathp3=(a,e,d).The original flow distribution pattern isno longer an equilibrium pattern, since atthis level of flow, the cost on path p3,Cp3=70.The new equilibrium flow patternnetwork is xp1

*= xp2*= xp3

*= 2.The equilibrium path travel cost isCp1=Cp2= Cp3= 92.

1

2 3

4

a b

c d

e

ce(fe)= fe+10

Page 52: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Four Demand Ranges

• Demand Range I: dw∊[0, 80/31)– Only p1 and p2 are used and the Braess Paradox does not

occur

• Demand Range II: dw∊ [80/31,40/11]– Only p1 and p2 are used and the Braess Paradox occurs

• Demand Range III: dw∊ (40/11,80/9]– All paths are used and the Braess Paradox still occurs

• Demand Range IV: dw∊ (80/9, ∞ )– Only p1 and p2 are used and the Braess Paradox vanishes

Page 53: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance and Ranking of Links andNodes in Demand Range I

Page 54: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance and Ranking of Links andNodes in Demand Range II

Page 55: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance and Ranking of Links andNodes in Demand Range III

Page 56: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance and Ranking of Links andNodes in Demand Range IV

Page 57: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance Ranking of Links in the Braess Network

0

1

2

3

4

a b c d e

Link

Ran

king

Importance Ranking inDemand Range IImportance Ranking inDemand Range IIImportance Ranking inDemand Range IIIImportance Ranking inDemand Range IV

Page 58: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance Ranking of Nodes in the Braess Network

0

1

2

3

1 2 3 4

Node

Ran

king

Importance Ranking inDemand Range IImportance Ranking inDemand Range IIImportance Ranking inDemand Range IIIImportance Ranking inDemand Range IV

Page 59: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Discussion

Links b and c are less important inDemand Range I than Demand RangeII, III and IV because they carry zeroflow in Demand Range I

Page 60: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Application II: the “Coupled” BraessNetwork

1

2

3

4

a

bc

d

e

6

5

7

h

g

k

lm

dw1=2 dw2=6

Page 61: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance and Ranking of Links

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Importance Ranking of Links in the Coupled Braess Network

0

1

2

3

4

5

6

7

a b c d e g h k l m

Link

Ran

king

ImportanceRanking ofLinks from theN-Q MeasureImportanceRanking ofLinks from theL-M Measure

Page 63: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance and Ranking of Nodes

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Importance Ranking of Nodes in the Coupled Braess Network

0

1

23

4

5

6

1 2 3 4 5 6 7

Node

Ran

king

ImportanceRanking from theN-Q MeasureImportanceRanking from theL-M Measure

Page 65: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Discussion

• Links l and g are the most important linksfrom the N-Q measure while they are only inthird place from the L-M measure becausethey carry a larger amount of flow.

• Links a and d are the most important linksfrom the L-M measure while they are only inthird place from the N-Q measure becausethey carry a less amount of flow.

Page 66: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Application III: An Electric Power SupplyChain Network

Nagurney and Liu (2006) and Nagurney,Liu, Cojocaru and Daniele (2005) haveshown that an electric power supplychain network can be transformed intoan equivalent transportation networkproblem.

Page 67: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Supernetwork Transformation

Example 1 from Nagurney, Liu, Cojocaru and Daniele, TRE (2005)

Page 68: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Five Demand Ranges

• Demand Range I: dw∊ [0, 1]• Demand Range II: dw∊ (1,4/3]• Demand Range III: dw∊ (4/3,7/3]• Demand Range IV: dw∊ (7/3, 11/3]• Demand Range V: dw∊ (11/3, ∞ )

Page 69: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance and Ranking of Links andNodes in Demand Range I

Page 70: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance and Ranking of Links andNodes in Demand Range II

Page 71: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance and Ranking of Links andNodes in Demand Range III

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Importance and Ranking of Links andNodes in Demand Range IV

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Importance and Ranking of Links andNodes in Demand Range V

Page 74: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance Ranking of Links in the Electric Power Supply Chain

Network

0

1

2

3

4

a b c d e f

Link

Ran

king

Importance Ranking inDemand Range IImportance Ranking inDemand Range IIImportance Ranking inDemand Range IIIImportance Ranking inDemand Range IVImportance Ranking inDemand Range V

Page 75: Transportation Science and the Dynamics of Critical ...supernet.isenberg.umass.edu/visuals/UMass_Civil_ Engineering_DEC… · Title: Transportation Science and the Dynamics of Critical

Importance Ranking of Nodes in the Electric Power Supply Chain

Network

0

1

2

3

4

Power

Gen

erato

r 1Pow

er S

uppli

er 1

Power

Sup

plier

2Pow

er S

uppli

er 3

Deman

d Mar

ket 1

Node

Ran

king

Importance Ranking inDemand Range IImportance Ranking inDemand Range IIImportance Ranking inDemand Range IIIImportance Ranking inDemand Range IVImportance Ranking inDemand Range V

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Discussion

Links a and d are the most important linksand power supplier 1 is ranked thesecond due to the fact that path p1,which consists of links a and d andpower supplier 1 carry the largestamount of flow.

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New Challengesand Opportunities: TheUnification of EVIs and

PDSs

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Bellagio ResearchTeam Residency

March 2004

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Double-Layered Dynamics

The unification of EVIs and PDSs allows themodeling of dynamic networks over different timescales.

Papers:Projected Dynamical Systems and Evolutionary Variational Inequalities

via Hilbert Spaces with Applications (Cojocaru, Daniele, and Nagurney),Journal of Optimization Theory and Applications, vol. 127, no. 3, pp. 1-15, December 2005.

Double-Layered Dynamics: A Unified Theory of Projected DynamicalSystems and Evolutionary Variational Inequalities (Cojocaru, Daniele,and Nagurney), European Journal of Operational Research, in press.

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A Pictorial of theDouble-Layered Dynamics

x(t1)

t=T

t=0

x(t1,0)

x(t2, 0)

x(t2)

x(t1, τ)

x(t2, τ)

PDSt1

PDSt2EVI

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There are new exciting questions, boththeoretical and computational, arising fromthis multiple time structure.

In the course of answering these questions, anew theory is taking shape from the synthesisof PDS and EVI, and, as such, it deserves aname of its own; we call it double-layereddynamics.

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Thank you!

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