Conditional Independence, Conditional Mixing and Conditional Association
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Mixing, Chaotic Advection, and Turbulence
Annual Reviews www.annualreviews.org/aronline Annu. Rev. Fluid Mech. 1990.22:207-53 Copyright © 1990 hV Annual Reviews Inc. All r~hts reserved MIXING, CHAOTIC ADVECTION, AND TURBULENCE J. M. Ottino Department of Chemical Engineering, University of Massachusetts, Amherst, Massachusetts 01003 1. INTRODUCTION 1.1 Setting The establishment of a paradigm for mixing of fluids can substantially affect the developmentof various branches of physical sciences and tech- nology. Mixing is intimately connected with turbulence, Earth and natural sciences, and various branches of engineering. However, in spite of its universality, there have been surprisingly few attempts to construct a general frameworkfor analysis. An examination of any library index reveals that there are almost no works textbooks or monographs focusing on the fluid mechanics of mixing from a global perspective. In fact, there have been few articles published in these pages devoted exclusively to mixing since the first issue in 1969 [one possible exception is Hill’s "Homogeneous Turbulent Mixing With Chemical Reaction" (1976), which is largely based on statistical theory]. However,mixing has been an important component in various other articles; a few of them are "Mixing-Controlled Supersonic Combustion" (Ferri 1973), "Turbulence and Mixing in Stably Stratified Waters" (Sherman et al. 1978), "Eddies, Waves, Circulation, and Mixing: Statistical Geofluid Mechanics" (Holloway 1986), and "Ocean Tur- bulence" (Gargett 1989). It is apparent that mixing appears in both indus- try and nature and the problems span an enormous range of time and length scales; the Reynolds numberin problems where mixing is important varies by 40 orders of magnitude(see Figure 1). -
Stat 8112 Lecture Notes Stationary Stochastic Processes Charles J
Stat 8112 Lecture Notes Stationary Stochastic Processes Charles J. Geyer April 29, 2012 1 Stationary Processes A sequence of random variables X1, X2, ::: is called a time series in the statistics literature and a (discrete time) stochastic process in the probability literature. A stochastic process is strictly stationary if for each fixed positive integer k the distribution of the random vector (Xn+1;:::;Xn+k) has the same distribution for all nonnegative integers n. A stochastic process having second moments is weakly stationary or sec- ond order stationary if the expectation of Xn is the same for all positive integers n and for each nonnegative integer k the covariance of Xn and Xn+k is the same for all positive integers n. 2 The Birkhoff Ergodic Theorem The Birkhoff ergodic theorem is to strictly stationary stochastic pro- cesses what the strong law of large numbers (SLLN) is to independent and identically distributed (IID) sequences. In effect, despite the different name, it is the SLLN for stationary stochastic processes. Suppose X1, X2, ::: is a strictly stationary stochastic process and X1 has expectation (so by stationary so do the rest of the variables). Write n 1 X X = X : n n i i=1 To introduce the Birkhoff ergodic theorem, it says a.s. Xn −! Y; (1) where Y is a random variable satisfying E(Y ) = E(X1). More can be said about Y , but we will have to develop some theory first. 1 The SSLN for IID sequences says the same thing as the Birkhoff ergodic theorem (1) except that in the SLLN for IID sequences the limit Y = E(X1) is constant. -
Pointwise and L1 Mixing Relative to a Sub-Sigma Algebra
POINTWISE AND L1 MIXING RELATIVE TO A SUB-SIGMA ALGEBRA DANIEL J. RUDOLPH Abstract. We consider two natural definitions for the no- tion of a dynamical system being mixing relative to an in- variant sub σ-algebra H. Both concern the convergence of |E(f · g ◦ T n|H) − E(f|H)E(g ◦ T n|H)| → 0 as |n| → ∞ for appropriate f and g. The weaker condition asks for convergence in L1 and the stronger for convergence a.e. We will see that these are different conditions. Our goal is to show that both these notions are robust. As is quite standard we show that one need only consider g = f and E(f|H) = 0, and in this case |E(f · f ◦ T n|H)| → 0. We will see rather easily that for L1 convergence it is enough to check an L2-dense family. Our major result will be to show the same is true for pointwise convergence making this a verifiable condition. As an application we will see that if T is mixing then for any ergodic S, S × T is relatively mixing with respect to the first coordinate sub σ-algebra in the pointwise sense. 1. Introduction Mixing properties for ergodic measure preserving systems gener- ally have versions “relative” to an invariant sub σ-algebra (factor algebra). For most cases the fundamental theory for the abso- lute case lifts to the relative case. For example one can say T is relatively weakly mixing with respect to a factor algebra H if 1) L2(µ) has no finite dimensional invariant submodules over the subspace of H-measurable functions, or Date: August 31, 2005. -
On Li-Yorke Measurable Sensitivity
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 143, Number 6, June 2015, Pages 2411–2426 S 0002-9939(2015)12430-6 Article electronically published on February 3, 2015 ON LI-YORKE MEASURABLE SENSITIVITY JARED HALLETT, LUCAS MANUELLI, AND CESAR E. SILVA (Communicated by Nimish Shah) Abstract. The notion of Li-Yorke sensitivity has been studied extensively in the case of topological dynamical systems. We introduce a measurable version of Li-Yorke sensitivity, for nonsingular (and measure-preserving) dynamical systems, and compare it with various mixing notions. It is known that in the case of nonsingular dynamical systems, a conservative ergodic Cartesian square implies double ergodicity, which in turn implies weak mixing, but the converses do not hold in general, though they are all equivalent in the finite measure- preserving case. We show that for nonsingular systems, an ergodic Cartesian square implies Li-Yorke measurable sensitivity, which in turn implies weak mixing. As a consequence we obtain that, in the finite measure-preserving case, Li-Yorke measurable sensitivity is equivalent to weak mixing. We also show that with respect to totally bounded metrics, double ergodicity implies Li-Yorke measurable sensitivity. 1. Introduction The notion of sensitive dependence for topological dynamical systems has been studied by many authors; see, for example, the works [3, 7, 10] and the references therein. Recently, various notions of measurable sensitivity have been explored in ergodic theory; see for example [2, 9, 11–14]. In this paper we are interested in formulating a measurable version of the topolog- ical notion of Li-Yorke sensitivity for the case of nonsingular and measure-preserving dynamical systems. -
Chaos Theory
By Nadha CHAOS THEORY What is Chaos Theory? . It is a field of study within applied mathematics . It studies the behavior of dynamical systems that are highly sensitive to initial conditions . It deals with nonlinear systems . It is commonly referred to as the Butterfly Effect What is a nonlinear system? . In mathematics, a nonlinear system is a system which is not linear . It is a system which does not satisfy the superposition principle, or whose output is not directly proportional to its input. Less technically, a nonlinear system is any problem where the variable(s) to be solved for cannot be written as a linear combination of independent components. the SUPERPOSITION PRINCIPLE states that, for all linear systems, the net response at a given place and time caused by two or more stimuli is the sum of the responses which would have been caused by each stimulus individually. So that if input A produces response X and input B produces response Y then input (A + B) produces response (X + Y). So a nonlinear system does not satisfy this principal. There are 3 criteria that a chaotic system satisfies 1) sensitive dependence on initial conditions 2) topological mixing 3) periodic orbits are dense 1) Sensitive dependence on initial conditions . This is popularly known as the "butterfly effect” . It got its name because of the title of a paper given by Edward Lorenz titled Predictability: Does the Flap of a Butterfly’s Wings in Brazil set off a Tornado in Texas? . The flapping wing represents a small change in the initial condition of the system, which causes a chain of events leading to large-scale phenomena. -
Turbulence, Fractals, and Mixing
Turbulence, fractals, and mixing Paul E. Dimotakis and Haris J. Catrakis GALCIT Report FM97-1 17 January 1997 Firestone Flight Sciences Laboratory Guggenheim Aeronautical Laboratory Karman Laboratory of Fluid Mechanics and Jet Propulsion Pasadena Turbulence, fractals, and mixing* Paul E. Dimotakis and Haris J. Catrakis Graduate Aeronautical Laboratories California Institute of Technology Pasadena, California 91125 Abstract Proposals and experimenta1 evidence, from both numerical simulations and laboratory experiments, regarding the behavior of level sets in turbulent flows are reviewed. Isoscalar surfaces in turbulent flows, at least in liquid-phase turbulent jets, where extensive experiments have been undertaken, appear to have a geom- etry that is more complex than (constant-D) fractal. Their description requires an extension of the original, scale-invariant, fractal framework that can be cast in terms of a variable (scale-dependent) coverage dimension, Dd(X). The extension to a scale-dependent framework allows level-set coverage statistics to be related to other quantities of interest. In addition to the pdf of point-spacings (in 1-D), it can be related to the scale-dependent surface-to-volume (perimeter-to-area in 2-D) ratio, as well as the distribution of distances to the level set. The application of this framework to the study of turbulent -jet mixing indicates that isoscalar geometric measures are both threshold and Reynolds-number dependent. As regards mixing, the analysis facilitated by the new tools, as well as by other criteria, indicates en- hanced mixing with increasing Reynolds number, at least for the range of Reynolds numbers investigated. This results in a progressively less-complex level-set geom- etry, at least in liquid-phase turbulent jets, with increasing Reynolds number. -
Cos513 Lecture 2 Conditional Independence and Factorization
COS513 LECTURE 2 CONDITIONAL INDEPENDENCE AND FACTORIZATION HAIPENG ZHENG, JIEQI YU Let {X1,X2, ··· ,Xn} be a set of random variables. Now we have a series of questions about them: • What are the conditional probabilities (answered by normalization / marginalization)? • What are the independencies (answered by factorization of the joint distribution)? For now, we assume that all random variables are discrete. Then the joint distribution is a table: (0.1) p(x1, x2, ··· , xn). Therefore, Graphic Model (GM) is a economic representation of joint dis- tribution taking advantage of the local relationships between the random variables. 1. DIRECTED GRAPHICAL MODELS (DGM) A directed GM is a Directed Acyclic Graph (DAG) G(V, E), where •V, the set of vertices, represents the random variables; •E, the edges, denotes the “parent of” relationships. We also define (1.1) Πi = set of parents of Xi. For example, in the graph shown in Figure 1.1, The random variables are X4 X4 X2 X2 X 6 X X1 6 X1 X3 X5 X3 X5 XZY XZY FIGURE 1.1. Example of Graphical Model 1 Y X Y Y X Y XZZ XZZ Y XYY XY XZZ XZZ XZY XZY 2 HAIPENG ZHENG, JIEQI YU {X1,X2 ··· ,X6}, and (1.2) Π6 = {X2,X3}. This DAG represents the following joint distribution: (1.3) p(x1:6) = p(x1)p(x2|x1)p(x3|x1)p(x4|x2)p(x5|x3)p(x6|x2, x5). In general, n Y (1.4) p(x1:n) = p(xi|xπi ) i=1 specifies a particular joint distribution. Note here πi stands for the set of indices of the parents of i. -
Data-Mining Probabilists Or Experimental Determinists?
Gopnik-CH_13.qxd 10/10/2006 1:39 PM Page 208 13 Data-Mining Probabilists or Experimental Determinists? A Dialogue on the Principles Underlying Causal Learning in Children Thomas Richardson, Laura Schulz, & Alison Gopnik This dialogue is a distillation of a real series of conver- Meno: Leaving aside the question of how children sations that took place at that most platonic of acade- learn for a while, can we agree on some basic prin- mies, the Center for Advanced Studies in the ciples for causal inference by anyone—child, Behavioral Sciences, between the first and third adult, or scientist? \edq1\ authors.\edq1\ The second author had determinist leanings to begin with and acted as an intermediary. Laplace: I think so. I think we can both generally agree that, subject to various caveats, two variables will not be dependent in probability unless there is Determinism, Faithfulness, and Causal some kind of causal connection present. Inference Meno: Yes—that’s what I’d call the weak causal Narrator: [Meno and Laplace stand in the corridor Markov condition. I assume that the kinds of of a daycare, observing toddlers at play through a caveats you have in mind are to restrict this princi- window.] ple to situations in which a discussion of cause and effect might be reasonable in the first place? Meno: Do you ever wonder how it is that children manage to learn so many causal relations so suc- Laplace: Absolutely. I don’t want to get involved in cessfully, so quickly? They make it all seem effort- discussions of whether X causes 2X or whether the less. -
Blocking Conductance and Mixing in Random Walks
Blocking conductance and mixing in random walks Ravindran Kannan Department of Computer Science Yale University L´aszl´oLov´asz Microsoft Research and Ravi Montenegro Georgia Institute of Technology Contents 1 Introduction 3 2 Continuous state Markov chains 7 2.1 Conductance and other expansion measures . 8 3 General mixing results 11 3.1 Mixing time estimates in terms of a parameter function . 11 3.2 Faster convergence to stationarity . 13 3.3 Constructing mixweight functions . 13 3.4 Explicit conductance bounds . 16 3.5 Finite chains . 17 3.6 Further examples . 18 4 Random walks in convex bodies 19 4.1 A logarithmic Cheeger inequality . 19 4.2 Mixing of the ball walk . 21 4.3 Sampling from a convex body . 21 5 Proofs I: Markov Chains 22 5.1 Proof of Theorem 3.1 . 22 5.2 Proof of Theorem 3.2 . 24 5.3 Proof of Theorem 3.3 . 26 1 6 Proofs II: geometry 27 6.1 Lemmas . 27 6.2 Proof of theorem 4.5 . 29 6.3 Proof of theorem 4.6 . 30 6.4 Proof of Theorem 4.3 . 32 2 Abstract The notion of conductance introduced by Jerrum and Sinclair [JS88] has been widely used to prove rapid mixing of Markov Chains. Here we introduce a bound that extends this in two directions. First, instead of measuring the conductance of the worst subset of states, we bound the mixing time by a formula that can be thought of as a weighted average of the Jerrum-Sinclair bound (where the average is taken over subsets of states with different sizes). -
Bayesian Networks
Bayesian Networks Read R&N Ch. 14.1-14.2 Next lecture: Read R&N 18.1-18.4 You will be expected to know • Basic concepts and vocabulary of Bayesian networks. – Nodes represent random variables. – Directed arcs represent (informally) direct influences. – Conditional probability tables, P( Xi | Parents(Xi) ). • Given a Bayesian network: – Write down the full joint distribution it represents. • Given a full joint distribution in factored form: – Draw the Bayesian network that represents it. • Given a variable ordering and some background assertions of conditional independence among the variables: – Write down the factored form of the full joint distribution, as simplified by the conditional independence assertions. Computing with Probabilities: Law of Total Probability Law of Total Probability (aka “summing out” or marginalization) P(a) = Σb P(a, b) = Σb P(a | b) P(b) where B is any random variable Why is this useful? given a joint distribution (e.g., P(a,b,c,d)) we can obtain any “marginal” probability (e.g., P(b)) by summing out the other variables, e.g., P(b) = Σa Σc Σd P(a, b, c, d) Less obvious: we can also compute any conditional probability of interest given a joint distribution, e.g., P(c | b) = Σa Σd P(a, c, d | b) = (1 / P(b)) Σa Σd P(a, c, d, b) where (1 / P(b)) is just a normalization constant Thus, the joint distribution contains the information we need to compute any probability of interest. Computing with Probabilities: The Chain Rule or Factoring We can always write P(a, b, c, … z) = P(a | b, c, …. -
Chaos and Chaotic Fluid Mixing
Snapshots of modern mathematics № 4/2014 from Oberwolfach Chaos and chaotic fluid mixing Tom Solomon Very simple mathematical equations can give rise to surprisingly complicated, chaotic dynamics, with be- havior that is sensitive to small deviations in the ini- tial conditions. We illustrate this with a single re- currence equation that can be easily simulated, and with mixing in simple fluid flows. 1 Introduction to chaos People used to believe that simple mathematical equations had simple solutions and complicated equations had complicated solutions. However, Henri Poincaré (1854–1912) and Edward Lorenz [4] showed that some remarkably simple math- ematical systems can display surprisingly complicated behavior. An example is the well-known logistic map equation: xn+1 = Axn(1 − xn), (1) where xn is a quantity (between 0 and 1) at some time n, xn+1 is the same quantity one time-step later and A is a given real number between 0 and 4. One of the most common uses of the logistic map is to model variations in the size of a population. For example, xn can denote the population of adult mayflies in a pond at some point in time, measured as a fraction of the maximum possible number the adult mayfly population can reach in this pond. Similarly, xn+1 denotes the population of the next generation (again, as a fraction of the maximum) and the constant A encodes the influence of various factors on the 1 size of the population (ability of pond to provide food, fraction of adults that typically reproduce, fraction of hatched mayflies not reaching adulthood, overall mortality rate, etc.) As seen in Figure 1, the behavior of the logistic system changes dramatically with changes in the parameter A. -
(Ω, F,P) Be a Probability Spac
Lecture 9: Independence, conditional independence, conditional distribution Definition 1.7. Let (Ω, F,P ) be a probability space. (i) Let C be a collection of subsets in F. Events in C are said to be independent if and only if for any positive integer n and distinct events A1,...,An in C, P (A1 ∩ A2 ∩···∩ An)= P (A1)P (A2) ··· P (An). (ii) Collections Ci ⊂ F, i ∈ I (an index set that can be uncountable), are said to be independent if and only if events in any collection of the form {Ai ∈ Ci : i ∈ I} are independent. (iii) Random elements Xi, i ∈ I, are said to be independent if and only if σ(Xi), i ∈ I, are independent. A useful result for checking the independence of σ-fields. Lemma 1.3. Let Ci, i ∈ I, be independent collections of events. Suppose that each Ci has the property that if A ∈ Ci and B ∈ Ci, then A∩B ∈ Ci. Then σ(Ci), i ∈ I, are independent. Random variables Xi, i =1, ..., k, are independent according to Definition 1.7 if and only if k F(X1,...,Xk)(x1, ..., xk)= FX1 (x1) ··· FXk (xk), (x1, ..., xk) ∈ R Take Ci = {(a, b] : a ∈ R, b ∈ R}, i =1, ..., k If X and Y are independent random vectors, then so are g(X) and h(Y ) for Borel functions g and h. Two events A and B are independent if and only if P (B|A) = P (B), which means that A provides no information about the probability of the occurrence of B. Proposition 1.11.