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Uncertain, High-Dimensional Dynamical Systems
Igor Mezić University of California, Santa Barbara IPAM, UCLA, February 2005
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Introduction Measure of uncertainty?
Uncertainty and spectral theory of dynamical systems. Model validation and data assimilation. Decompositions.
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Dynamical evolution of uncertainty: an example
Output measure Input measure Bifurcation increases uncertainty, but how? Tradeoff: Bifurcation vs. contracting dynamics
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Dynamical evolution of uncertainty: general set-up
Skew-product system.
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Dynamical evolution of uncertainty: general set-up
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Dynamical evolution of uncertainty: general set-up
F(z) 1 f T
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Dynamical evolution of uncertainty: simple examples
Fw(z) 1 Expanding maps: x’=2x
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A measure of uncertainty of an observable
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Computation of uncertainty in CDF metric
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Maximal uncertainty for CDF metric
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Variance, Entropy and Uncertainty in CDF metric
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Uncertainty in CDF metric: Pitchfork bifurcation
x Output measure Input measure
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Time-averaged uncertainty
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Conclusions
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Introduction PV=NkT Example: thermodynamics from statistical mechanics
“…Any rarified gas will behave that way, no matter how queer the dynamics of its particles…” Goodstein (1985) Example: Galerkin truncation of evolution equations. Information comes from a single observable time-series.
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Introduction When do two dynamical systems exhibit similar behavior?
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Introduction Constructive proof that ergodic partitions and invariant
measures of systems can be compared using a single observable (“Statistical Takens-Aeyels” theorem). A formalism based on harmonic analysis that extends the concept of comparing the invariant measure.
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Set-up Time averages and invariant measures:
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Set-up
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Pseudometrics for Dynamical Systems
Pseudometric that captures statistics: where
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Ergodic partition
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Ergodic partition
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An example: analysis of experimental data
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Analysis of experimental data
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Analysis of experimental data
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Koopman operator, triple decomposition, MOD
-Efficient representation of the flow field; can be done with vectors -Lagrangian analysis: FLUCTUATIONS MEAN FLOW PERIODIC APERIODIC Desirable: “Triple decomposition”:
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Embedding
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Conclusions Constructive proof that ergodic partitions and invariant
measures of systems can be compared using a single observable –deterministic+stochastic. A formalism based on harmonic analysis that extends the concept of comparing the invariant measure Pseudometrics on spaces of dynamical systems. Statistics – based, linear (but infinite-dimensional).
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Introduction Everson et al., JPO 27 (1997)
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Introduction 4 modes -99% of the variance! -no dynamics!
Everson et al., JPO 27 (1997)
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Introduction In this talk:
-Account explicitly for dynamics to produce a decomposition. -Tool: lift to infinite-dimensional space of functions on attractor + consider properties of Koopman operator. -Allows for detailed comparison of dynamical properties of the evolution and retained modes. -Split into “deterministic” and “stochastic” parts: useful for prediction purposes.
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Factors and harmonic analysis
Example:
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Factors and harmonic analysis
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Harmonic analysis: an example
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Evolution equations and Koopman operator
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Evolution equations and Koopman operator
Similar:“Wold decomposition”
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Evolution equations and Koopman operator
But how to get this from data?
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Evolution equations and Koopman operator
is almost-periodic. -Remainder has continuous spectrum!
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Conclusions -Use properties of the Koopman operator to produce a decomposition -Tool: lift to infinite-dimensional space of functions on attractor. -Allows for detailed comparison of dynamical properties of the evolution and retained modes. -Split into “deterministic” and “stochastic” parts: useful for prediction purposes. -Useful for Lagrangian studies in fluid mechanics.
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Invariant measures and time-averages
Example: Probability histograms! -1 a1 a2 But poor for dynamics: Irrational a’s produce the same statistics
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Dynamical evolution of uncertainty: simple examples
Types of uncertainty: Epistemic (reducible) Aleatory (irreducible) A-priori (initial conditions, parameters, model structure) A-posteriori (chaotic dynamics, observation error) Expanding maps: x’=2x
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Uncertainty in CDF metric: Examples
Uncertainty strongly dependent on distribution of initial conditions.
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