some figures adapted from a 2004 lecture by larry liebovitch, ph.d. chaos biol/cmsc 361: emergence...
TRANSCRIPT
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Some figures adapted from a 2004 Lecture by Larry Liebovitch, Ph.D.ChaosBIOL/CMSC 361: Emergence1/29/08
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EmergenceNon-linearCoherenceDynamicSelf-OrganizationComplexityMacro-level Property (Structured)UnexpectedUnpredictable
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Properties of ChaosDeterministicSmall Number of Variables Complex OutputBifurcationsAttractorsSensitive to Initial ConditionsForecasting Uncertainty grows ExponentiallyPhase Space is Low Dimensional
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Deterministicpredict that valuethese valuesA future state fully determined by previous states Chaos: future states fully determined by initial state
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RandomA process or system whose behavior is Stochastic;without definite aim, reason or pattern;Whose outcome is described by a probability distribution.
Probability: relative possibility that an event will occur
Stochastic: a non-deterministic process
Deterministic: a prior state fully determines the future state of the process or system
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MeanVariancePower SpectrumRandomChaotic
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RandomData 1x(n) = rand()
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ChaosData 2
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Properties of ChaosDeterministicSmall Number of Variables Complex OutputBifurcationsAttractorsSensitive to Initial ConditionsForecasting Uncertainty grows ExponentiallyPhase Space is Low Dimensional
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Population Growth
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Bifurcation DiagramChoose a constant starting value for x (x0=0.1)
Choose a starting value for the rate (r = 0)
Use the equation to compute successive values of x(n) from prior values up to x(1000)
Ignore the first 900 values of x; these are transient values (before system stablizes)
Plot x(901) to x(1000) on the Y-axis versus the current value for r
Change the value of r and repeat
ZeroSteadyChaos
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Bifurcations
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Attractors
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Another Example
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Lorenz: Convection1963. J. Atmos. Sci. 20:13-141COLDModelHOT
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Lorenz EquationsX(t)Z(t)Y(t)
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Lorenz EquationsX = speed, direction of the convection circulationX > 0 clockwiseX < 0 counterclockwiseY = temperature difference between rising and falling fluidZ = rate of temperature change through fluid column
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Lorenz EquationsPhase SpaceZXY
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Sensitivity to Initial ConditionsX(t)X= 1.00001Initial Condition:differentsameX(t)X= 1.00
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Lorenz AttractorsX < 0X > 0cylinder of air rotating counter-clockwisecylinder of air rotating clockwise
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Why an Attractor?Trajectories from outside:pulled TOWARDS itwhy its called an attractorstarting away:
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Why Strange?strangenot strange
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Lorenz Strange AttractorTrajectories on the attractor:pushed APART from each othersensitivity to initial conditionsstarting on:
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Properties of ChaosDeterministicSmall Number of Variables Complex OutputBifurcationsAttractorsSensitive to Initial ConditionsForecasting Uncertainty grows ExponentiallyPhase Space is Low Dimensional
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Sensitivitynearly identicalinitial valuesvery differentfinal valuesor...very different behaviors...
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Sensitivitysmall change in a parameterone patternanother pattern
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Non-Chaotic Systemsystem outputcontrol parameter
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Chaotic Systemsystem outputcontrol parameter
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Clockwork UniverseInitial Conditions X(t0), Y(t0), Z(t0)...Cancomputeall futureX(t), Y(t), Z(t)...Equations
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Chaotic UniverseInitial Conditions X(t0), Y(t0), Z(t0)...sensitivityto initial conditionsCan notcomputeall futureX(t), Y(t), Z(t)...Equations
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Shadowing Theorem: Non-ChaoticIf the errors at each integration step are small, there is an EXACT trajectory which lies within a small distance of the errorfull trajectory that we calculated.CalculatedTrue
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Shadowing Theorem: ChaoticThere is an INFINITE number of trajectories. Were on an exact trajectory, just not on the one we thought we were on.CalculatedExpected
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Deterministic: ChaoticX(n+1) = f {X(n)}Accuracy of values computed for X(n):3.455 3.45? 3.4?? 3.??? ? ? ?
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Why?Sensitivity to initial conditions means that the conditions of an experiment can be quite similar, but that the results can be quite different a little initial error has a large impact!
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4. We are on a real trajectory.3. Pulled backtowards the attractor.2. Error pushesus offthe attractor.1. We start here.Trajectorythat we actuallycompute.Trajectory that we are trying to compute.
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Properties of ChaosDeterministicSmall Number of Variables Complex OutputBifurcationsAttractorsSensitive to Initial ConditionsForecasting Uncertainty grows ExponentiallyPhase Space is Low Dimensional
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Mechanism?ChanceDeterminism
Datax(t)t?
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Mechanism?Chanced(phase space set)Determinismd(phase space set) = lowDatax(t)t?
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ProcedureDetermine topological properties of the objectFractal Dimension
High Fractal Dimension RandomLow Fractal Dimension ChaoticFractal Dimension does not equalFractal Dimension
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ProcedureDetermine the Topological Properties of this ObjectEspecially, the fractal dimension.
High Fractal Dimension = Random = chance Low Fractal Dimension = Chaos = deterministic
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Fractal DimensionA measure of self similarityXtimed
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Fractal Dimension:The Dimension of the Attractor in Phase Space is related to theNumber of Independent Variables. Xtimedx(t)x(t+ t)x(t+2 t)
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Mechanism that generated the experimental data.DeterministicRandomd = lowd The fractal dimension of the phase space set tells us if the data was generated by a random or a deterministic mechanism.