An Introduction to Dynamical Systems Richard J. Brown
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The Topological Entropy Conjecture
mathematics Article The Topological Entropy Conjecture Lvlin Luo 1,2,3,4 1 Arts and Sciences Teaching Department, Shanghai University of Medicine and Health Sciences, Shanghai 201318, China; [email protected] or [email protected] 2 School of Mathematical Sciences, Fudan University, Shanghai 200433, China 3 School of Mathematics, Jilin University, Changchun 130012, China 4 School of Mathematics and Statistics, Xidian University, Xi’an 710071, China Abstract: For a compact Hausdorff space X, let J be the ordered set associated with the set of all finite open covers of X such that there exists nJ, where nJ is the dimension of X associated with ¶. Therefore, we have Hˇ p(X; Z), where 0 ≤ p ≤ n = nJ. For a continuous self-map f on X, let a 2 J be f an open cover of X and L f (a) = fL f (U)jU 2 ag. Then, there exists an open fiber cover L˙ f (a) of X induced by L f (a). In this paper, we define a topological fiber entropy entL( f ) as the supremum of f ent( f , L˙ f (a)) through all finite open covers of X = fL f (U); U ⊂ Xg, where L f (U) is the f-fiber of − U, that is the set of images f n(U) and preimages f n(U) for n 2 N. Then, we prove the conjecture log r ≤ entL( f ) for f being a continuous self-map on a given compact Hausdorff space X, where r is the maximum absolute eigenvalue of f∗, which is the linear transformation associated with f on the n L Cechˇ homology group Hˇ ∗(X; Z) = Hˇ i(X; Z). -
A Gentle Introduction to Dynamical Systems Theory for Researchers in Speech, Language, and Music
A Gentle Introduction to Dynamical Systems Theory for Researchers in Speech, Language, and Music. Talk given at PoRT workshop, Glasgow, July 2012 Fred Cummins, University College Dublin [1] Dynamical Systems Theory (DST) is the lingua franca of Physics (both Newtonian and modern), Biology, Chemistry, and many other sciences and non-sciences, such as Economics. To employ the tools of DST is to take an explanatory stance with respect to observed phenomena. DST is thus not just another tool in the box. Its use is a different way of doing science. DST is increasingly used in non-computational, non-representational, non-cognitivist approaches to understanding behavior (and perhaps brains). (Embodied, embedded, ecological, enactive theories within cognitive science.) [2] DST originates in the science of mechanics, developed by the (co-)inventor of the calculus: Isaac Newton. This revolutionary science gave us the seductive concept of the mechanism. Mechanics seeks to provide a deterministic account of the relation between the motions of massive bodies and the forces that act upon them. A dynamical system comprises • A state description that indexes the components at time t, and • A dynamic, which is a rule governing state change over time The choice of variables defines the state space. The dynamic associates an instantaneous rate of change with each point in the state space. Any specific instance of a dynamical system will trace out a single trajectory in state space. (This is often, misleadingly, called a solution to the underlying equations.) Description of a specific system therefore also requires specification of the initial conditions. In the domain of mechanics, where we seek to account for the motion of massive bodies, we know which variables to choose (position and velocity). -
A Cell Dynamical System Model for Simulation of Continuum Dynamics of Turbulent Fluid Flows A
A Cell Dynamical System Model for Simulation of Continuum Dynamics of Turbulent Fluid Flows A. M. Selvam and S. Fadnavis Email: [email protected] Website: http://www.geocities.com/amselvam Trends in Continuum Physics, TRECOP ’98; Proceedings of the International Symposium on Trends in Continuum Physics, Poznan, Poland, August 17-20, 1998. Edited by Bogdan T. Maruszewski, Wolfgang Muschik, and Andrzej Radowicz. Singapore, World Scientific, 1999, 334(12). 1. INTRODUCTION Atmospheric flows exhibit long-range spatiotemporal correlations manifested as the fractal geometry to the global cloud cover pattern concomitant with inverse power-law form for power spectra of temporal fluctuations of all scales ranging from turbulence (millimeters-seconds) to climate (thousands of kilometers-years) (Tessier et. al., 1996) Long-range spatiotemporal correlations are ubiquitous to dynamical systems in nature and are identified as signatures of self-organized criticality (Bak et. al., 1988) Standard models for turbulent fluid flows in meteorological theory cannot explain satisfactorily the observed multifractal (space-time) structures in atmospheric flows. Numerical models for simulation and prediction of atmospheric flows are subject to deterministic chaos and give unrealistic solutions. Deterministic chaos is a direct consequence of round-off error growth in iterative computations. Round-off error of finite precision computations doubles on an average at each step of iterative computations (Mary Selvam, 1993). Round- off error will propagate to the mainstream computation and give unrealistic solutions in numerical weather prediction (NWP) and climate models which incorporate thousands of iterative computations in long-term numerical integration schemes. A recently developed non-deterministic cell dynamical system model for atmospheric flows (Mary Selvam, 1990; Mary Selvam et. -
Chapter 5. Flow Maps and Dynamical Systems
Chapter 5 Flow Maps and Dynamical Systems Main concepts: In this chapter we introduce the concepts of continuous and discrete dynamical systems on phase space. Keywords are: classical mechanics, phase space, vector field, linear systems, flow maps, dynamical systems Figure 5.1: A solar system is well modelled by classical mechanics. (source: Wikimedia Commons) In Chapter 1 we encountered a variety of ODEs in one or several variables. Only in a few cases could we write out the solution in a simple closed form. In most cases, the solutions will only be obtainable in some approximate sense, either from an asymptotic expansion or a numerical computation. Yet, as discussed in Chapter 3, many smooth systems of differential equations are known to have solutions, even globally defined ones, and so in principle we can suppose the existence of a trajectory through each point of phase space (or through “almost all” initial points). For such systems we will use the existence of such a solution to define a map called the flow map that takes points forward t units in time from their initial points. The concept of the flow map is very helpful in exploring the qualitative behavior of numerical methods, since it is often possible to think of numerical methods as approximations of the flow map and to evaluate methods by comparing the properties of the map associated to the numerical scheme to those of the flow map. 25 26 CHAPTER 5. FLOW MAPS AND DYNAMICAL SYSTEMS In this chapter we will address autonomous ODEs (recall 1.13) only: 0 d y = f(y), y, f ∈ R (5.1) 5.1 Classical mechanics In Chapter 1 we introduced models from population dynamics. -
Thermodynamic Properties of Coupled Map Lattices 1 Introduction
Thermodynamic properties of coupled map lattices J´erˆome Losson and Michael C. Mackey Abstract This chapter presents an overview of the literature which deals with appli- cations of models framed as coupled map lattices (CML’s), and some recent results on the spectral properties of the transfer operators induced by various deterministic and stochastic CML’s. These operators (one of which is the well- known Perron-Frobenius operator) govern the temporal evolution of ensemble statistics. As such, they lie at the heart of any thermodynamic description of CML’s, and they provide some interesting insight into the origins of nontrivial collective behavior in these models. 1 Introduction This chapter describes the statistical properties of networks of chaotic, interacting el- ements, whose evolution in time is discrete. Such systems can be profitably modeled by networks of coupled iterative maps, usually referred to as coupled map lattices (CML’s for short). The description of CML’s has been the subject of intense scrutiny in the past decade, and most (though by no means all) investigations have been pri- marily numerical rather than analytical. Investigators have often been concerned with the statistical properties of CML’s, because a deterministic description of the motion of all the individual elements of the lattice is either out of reach or uninteresting, un- less the behavior can somehow be described with a few degrees of freedom. However there is still no consistent framework, analogous to equilibrium statistical mechanics, within which one can describe the probabilistic properties of CML’s possessing a large but finite number of elements. -
Writing the History of Dynamical Systems and Chaos
Historia Mathematica 29 (2002), 273–339 doi:10.1006/hmat.2002.2351 Writing the History of Dynamical Systems and Chaos: View metadata, citation and similar papersLongue at core.ac.uk Dur´ee and Revolution, Disciplines and Cultures1 brought to you by CORE provided by Elsevier - Publisher Connector David Aubin Max-Planck Institut fur¨ Wissenschaftsgeschichte, Berlin, Germany E-mail: [email protected] and Amy Dahan Dalmedico Centre national de la recherche scientifique and Centre Alexandre-Koyre,´ Paris, France E-mail: [email protected] Between the late 1960s and the beginning of the 1980s, the wide recognition that simple dynamical laws could give rise to complex behaviors was sometimes hailed as a true scientific revolution impacting several disciplines, for which a striking label was coined—“chaos.” Mathematicians quickly pointed out that the purported revolution was relying on the abstract theory of dynamical systems founded in the late 19th century by Henri Poincar´e who had already reached a similar conclusion. In this paper, we flesh out the historiographical tensions arising from these confrontations: longue-duree´ history and revolution; abstract mathematics and the use of mathematical techniques in various other domains. After reviewing the historiography of dynamical systems theory from Poincar´e to the 1960s, we highlight the pioneering work of a few individuals (Steve Smale, Edward Lorenz, David Ruelle). We then go on to discuss the nature of the chaos phenomenon, which, we argue, was a conceptual reconfiguration as -
Role of Nonlinear Dynamics and Chaos in Applied Sciences
v.;.;.:.:.:.;.;.^ ROLE OF NONLINEAR DYNAMICS AND CHAOS IN APPLIED SCIENCES by Quissan V. Lawande and Nirupam Maiti Theoretical Physics Oivisipn 2000 Please be aware that all of the Missing Pages in this document were originally blank pages BARC/2OOO/E/OO3 GOVERNMENT OF INDIA ATOMIC ENERGY COMMISSION ROLE OF NONLINEAR DYNAMICS AND CHAOS IN APPLIED SCIENCES by Quissan V. Lawande and Nirupam Maiti Theoretical Physics Division BHABHA ATOMIC RESEARCH CENTRE MUMBAI, INDIA 2000 BARC/2000/E/003 BIBLIOGRAPHIC DESCRIPTION SHEET FOR TECHNICAL REPORT (as per IS : 9400 - 1980) 01 Security classification: Unclassified • 02 Distribution: External 03 Report status: New 04 Series: BARC External • 05 Report type: Technical Report 06 Report No. : BARC/2000/E/003 07 Part No. or Volume No. : 08 Contract No.: 10 Title and subtitle: Role of nonlinear dynamics and chaos in applied sciences 11 Collation: 111 p., figs., ills. 13 Project No. : 20 Personal authors): Quissan V. Lawande; Nirupam Maiti 21 Affiliation ofauthor(s): Theoretical Physics Division, Bhabha Atomic Research Centre, Mumbai 22 Corporate authoifs): Bhabha Atomic Research Centre, Mumbai - 400 085 23 Originating unit : Theoretical Physics Division, BARC, Mumbai 24 Sponsors) Name: Department of Atomic Energy Type: Government Contd...(ii) -l- 30 Date of submission: January 2000 31 Publication/Issue date: February 2000 40 Publisher/Distributor: Head, Library and Information Services Division, Bhabha Atomic Research Centre, Mumbai 42 Form of distribution: Hard copy 50 Language of text: English 51 Language of summary: English 52 No. of references: 40 refs. 53 Gives data on: Abstract: Nonlinear dynamics manifests itself in a number of phenomena in both laboratory and day to day dealings. -
Flows of Continuous-Time Dynamical Systems with No Periodic Orbit As an Equivalence Class Under Topological Conjugacy Relation
Journal of Mathematics and Statistics 7 (3): 207-215, 2011 ISSN 1549-3644 © 2011 Science Publications Flows of Continuous-Time Dynamical Systems with No Periodic Orbit as an Equivalence Class under Topological Conjugacy Relation Tahir Ahmad and Tan Lit Ken Department of Mathematics, Faculty of Science, Nanotechnology Research Alliance, Theoretical and Computational Modeling for Complex Systems, University Technology Malaysia 81310 Skudai, Johor, Malaysia Abstract: Problem statement: Flows of continuous-time dynamical systems with the same number of equilibrium points and trajectories, and which has no periodic orbit form an equivalence class under the topological conjugacy relation. Approach: Arbitrarily, two trajectories resulting from two distinct flows of this type of dynamical systems were written as a set of points (orbit). A homeomorphism which maps between these two sets is then built. Using the notion of topological conjugacy, they were shown to conjugate topologically. By the arbitrariness in selection of flows and their respective initial states, the results were extended to all the flows of dynamical system of that type. Results: Any two flows of such dynamical systems were shown to share the same dynamics temporally along with other properties such as order isomorphic and homeomorphic. Conclusion: Topological conjugacy serves as an equivalence relation in the set of flows of continuous-time dynamical systems which have same number of equilibrium points and trajectories, and has no periodic orbit. Key words: Dynamical system, equilibrium points, trajectories, periodic orbit, equivalence class, topological conjugacy, order isomorphic, Flat Electroencephalography (Flat EEG), dynamical systems INTRODUCTION models. Nandhakumar et al . (2009) for example, the dynamics of robot arm is studied. -
Nonlinear Elasticity in a Deforming Ambient Space Contents 1
Nonlinear Elasticity in a Deforming Ambient Space∗ Arash Yavari† Arkadas Ozakin‡ Souhayl Sadik§ 27 May 2016 Abstract In this paper we formulate a nonlinear elasticity theory in which the ambient space is evolving. For a continuum moving in an evolving ambient space, we model time dependency of the metric by a time- dependent embedding of the ambient space in a larger manifold with a fixed background metric. We derive both the tangential and the normal governing equations. We then reduce the standard energy balance written in the larger ambient space to that in the evolving ambient space. We consider quasi-static deformations of the ambient space and show that a quasi-static deformation of the ambient space results in stresses, in general. We linearize the nonlinear theory about a reference motion and show that variation of the spatial metric corresponds to an effective field of body forces. Keywords: Geometric mechanics, nonlinear elasticity, deforming ambient space. Contents 1 Introduction 1 2 Motion of an Elastic Body in an Evolving Ambient Space3 2.1 Lagrangian Field Theory of Elasticity in an Evolving Ambient Space................3 2.2 Conservation of Mass for Motion in an Evolving Ambient Space................... 10 2.3 Energy Balance in Nonlinear Elasticity in an Evolving Ambient Space................ 11 3 Quasi-Static Deformations of the Ambient Space Metric 14 3.1 Examples of elastic bodies in evolving ambient spaces and the induced stresses.......... 14 3.2 Elastic deformations due to linear perturbations of the ambient space metric............ 20 A Geometry of Riemannian Submanifolds 24 B An Alternative Derivation of the Tangent Balance of Linear Momentum 27 1 Introduction In the geometric theory of elasticity, an elastic body is represented by a material manifold B , which defines the natural, stress-free state of the body. -
Persistence Stability for Geometric Complexes Arxiv:1207.3885V3
Persistence stability for geometric complexes Fr´ed´ericChazal∗, Vin de Silvay, Steve Oudotz November 11, 2013 Abstract In this paper we study the properties of the homology of different geometric filtered complexes (such as Vietoris{Rips, Cechˇ and witness complexes) built on top of totally bounded metric spaces. Using recent developments in the theory of topological persis- tence, we provide simple and natural proofs of the stability of the persistent homology of such complexes with respect to the Gromov–Hausdorff distance. We also exhibit a few noteworthy properties of the homology of the Rips and Cechˇ complexes built on top of compact spaces. 1 Introduction The inference of topological properties of metric spaces from approximations is a problem that has attracted special attention in computational topology in recent years. Given a metric space (Y; dY ) approximating an unknown metric space (X; dX ), the aim is to build a simplicial complex on the vertex set Y whose homology or homotopy type is the same as X. Note that, although Y is finite in many applications, finiteness is not a requirement a priori. Among the many geometric complexes available to us, the Vietoris{Rips complex (or simply `Rips complex') is particularly useful, being easy to compute and having good approximation arXiv:1207.3885v3 [math.AT] 15 Nov 2013 properties. We recall the definition. Let (X; dx) be a metric space and α a real parameter (the `scale'). Then Rips(X; α) is the simplical complex on X whose simplices are the finite subsets of X with diameter at most α: σ = [x0; x1; : : : ; xk] Rips(X; α) dX (xi; xj) α for all i; j 2 , ≤ ∗[email protected] [email protected] [email protected] 1 When (X; dX ) is a closed Riemannian manifold, J.-C. -
On Orbit Configuration Spaces of Spheres
CORE Metadata, citation and similar papers at core.ac.uk Provided by Elsevier - Publisher Connector Topology and its Applications 118 (2002) 85–102 On orbit configuration spaces of spheres Eva Maria Feichtner a,∗, Günter M. Ziegler b,∗ a Departement Mathematik, ETH Zürich, 8092 Zürich, Switzerland b Fachbereich Mathematik, MA 6-2, TU Berlin, 10623 Berlin, Germany Received 26 January 2000; received in revised form 10 July 2000 Abstract k The orbit configuration space FZ2 (S ,n) is the space of all ordered n-tuples of points on the k k-sphere such that no two of them are identical or antipodal. The cohomology algebra of FZ2 (S ,n), with integer coefficients, is here determined completely, and described in terms of generators, bases and relations. To this end, we analyze the cohomology spectral sequence of a fibration k → k FZ2 (S ,n) S , where the fiber—in contrast to the situation for the classical configuration space F(Sk,n)—is not the complement of a linear subspace arrangement. Analogies to the arrangement case, however, are crucial for getting a complete description of its cohomology. 2002 Elsevier Science B.V. All rights reserved. Keywords: Orbit configuration spaces; Integral cohomology algebra; Subspace arrangements; Leray–Serre spectral sequence 1. Introduction The ordered configuration spaces n F(M, n) := (x1,x2,...,xn) ∈ M : xi = xj for all i = j of a manifold M were first studied by Fadell and Neuwirth [15] in 1962. The cohomology of such spaces has received a lot of attention, at least since the work by Arnol’d [1] related to Hilbert’s 13th problem. -
Entropy: a Guide for the Perplexed 117 a Quasistatic Irreversible Path, and Then Go Back from B to a Along a Quasistatic Reversible Path
5 ENTROPY A GUIDE FOR THE PERPLEXED Roman Frigg and Charlotte Werndl1 1 Introduction Entropy is ubiquitous in physics, and it plays important roles in numerous other disciplines ranging from logic and statistics to biology and economics. However, a closer look reveals a complicated picture: entropy is defined differently in different contexts, and even within the same domain different notions of entropy are at work. Some of these are defined in terms of probabilities, others are not. The aim of this essay is to arrive at an understanding of some of the most important notions of entropy and to clarify the relations between them. In particular, we discuss the question what kind of probabilities are involved whenever entropy is defined in terms of probabilities: are the probabilities chances (i.e. physical probabilities) or credences (i.e. degrees of belief)? After setting the stage by introducing the thermodynamic entropy (Sec. 2), we discuss notions of entropy in information theory (Sec. 3), statistical mechanics (Sec. 4), dynamical-systems theory (Sec. 5), and fractal geometry (Sec. 6). Omis- sions are inevitable; in particular, space constraints prevent us from discussing entropy in quantum mechanics and cosmology.2 2 Entropy in thermodynamics Entropy made its first appearance in the middle of the nineteenth century in the context of thermodynamics (TD). TD describes processes like the exchange of heat between two bodies or the spreading of gases in terms of macroscopic variables like temperature, pressure, and volume. The centerpiece of TD is the Second Law of TD, which, roughly speaking, restricts the class of physically allowable processes in isolated systems to those that are not entropy-decreasing.