DOCSLIB.ORG

Stability Analysis of Complex Dynamical Systems: Some Computational Methods Narotham Reddy Sarabudla Iowa State University

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Stability Analysis of Complex Dynamical Systems: Some Computational Methods Narotham Reddy Sarabudla Iowa State University Iowa State University Capstones, Theses and Retrospective Theses and Dissertations Dissertations 1981 Stability analysis of complex dynamical systems: some computational methods Narotham Reddy Sarabudla Iowa State University Follow this and additional works at: https://lib.dr.iastate.edu/rtd Part of the Electrical and Electronics Commons Recommended Citation Sarabudla, Narotham Reddy, "Stability analysis of complex dynamical systems: some computational methods " (1981). Retrospective Theses and Dissertations. 6944. https://lib.dr.iastate.edu/rtd/6944 This Dissertation is brought to you for free and open access by the Iowa State University Capstones, Theses and Dissertations at Iowa State University Digital Repository. It has been accepted for inclusion in Retrospective Theses and Dissertations by an authorized administrator of Iowa State University Digital Repository. For more information, please contact [email protected]. INFORMATION TO USERS This was produced from a copy of a document sent to us for microfilming. While the most advanced technological means to photograph and reproduce this document have been used, the quality is heavily dependent upon the quality of the material submitted. The following explanation of techniques is provided to help you understand markings or notations which may appear on this reproduction. 1. The sign or "target" for pages apparently lacking from the document photographed is "Missing Page(s)". If it was possible to obtain the missing page(s) or section, they are spliced into the film along with adjacent pages. This may have necessitated cutting through an image and duplicating adjacent pages to assure you of complete continuity. 2. When an image on the film is obliterated with a round black mark it is an indication that the film inspector noticed either blurred copy because of movement during exposure, or duplicate copy. Unless we meant to delete copyrighted materials that should not have been filmed, you will find a good image of the page in the adjacent frame. If copyrighted materials were deleted you will find a target note listing the pages in the adjacent frame. 3. When a map, drawing or chart, etc., is part of the material being photo­ graphed the photographer has followed a definite method in "sectioning" the material. It is customary to begin filming at the upper left hand corner of a large sheet and to continue from left to right in equal sections with small overlaps. If necessary, sectioning is continued again—beginning below the first row and continuing on until complete. 4. For any illustrations that cannot be reproduced satisfactorily by xerography, photographic prints can be purchased at additional cost and tipped into your ' xerographic copy. Requests can be made to our Dissertations Customer Services Department. 5. Some pages in any document may have indistinct print. In all cases we have filmed the best available copy. Universi^ Mioxïilms International 300 N. ZEEB RD., ANN ARBOR, Ml 48106 8128855 SARABUDLA, NAROIHAM REDDY STABILITY ANALYSIS OF COMPLEX DYNAMICAL SYSTEMS: SOME COMPUTATIONAL METHODS Iowa State University PH.D. 1981 University Microfilms I ntsrnâtionâl 300 N. Zeeb Road, Am Arbor, Ml 48106 PLEASE NOTE: In all cases this material has been filmed in the best possible way from the available copy. Problems encountered with this document have been identified here with a check mark V . 1. Glossy photographs or pages ___ 2. Colored illustrations, paper or print 3. Photographs with dark background 4. Illustrations are poor copy 5. Pages with black marks, not original copy 6. Print shows through as there is text on both sides of page 7. Indistinct, broken or small print on several pages 8. Print exceeds margin requirements 9. Tightly bound copy with print lost in spine 10. Computer printout pages with indistinct print 11. Page(s) • lacking when material received, and not available from school or author. 12. Page(s) seem to be missing in numbering only as text follows. 13. Two pages numbered . Text follows. 14. Curling and wrinkled pages 15. Other University Microfilms International Stability analysis of complex dynamical systems; Some computational methods by Narotham Reddy Sarabudla A Dissertation Submitted to the Graduate Faculty in Partial Fulfillment of the Requirements for the Degree of DOCTOR OF PHILOSOPHY Department; Electrical Engineering Major; Electrical Engineering Approved; Signature was redacted for privacy. In Chaafge of Major Work Signature was redacted for privacy. r Department Signature was redacted for privacy. Iowa State University Ames, Iowa 1981 ii TABLE OF CONTEOTS Page I. INTRODUCTION 1 II. NOTATION 4 III. STABILITY THEORY 6 A, Lyapunov Stability Theory 7 1, Indirect method 7 2. Direct method 8 B, Constructive Stability Results 10 C, Domain of Attraction 16 IV. ANALYSIS BY QUADRATIC LYAPUNOV FUNCTIONS 20 A. Development of the Algorithm 20 B. Summary of the Algorithm 31 C. Discussion 32 D. Examples 36 E. Relationship Between the Eigenvalues of Jacobian and Lyapunov Matrices. 54 V. ANALYSIS BY NORt^ LYAPUNOV FUNCTIONS 60 A. Development of the Algorithm 60 B. Summary of the Algorithm 65 C. Discussion 66 ill Page VI. APPLICATION OF THE COMPARISON PRINCIPLE 69 A. Comparison Principle 71 B. Estimation of the Domain of Attraction 75 C. Discussion 83 VII. CONCLUSIONS ' 85 VIII. REFERENCES 88 IX. ACKNOTVLEDGMENTS 93 X. APPENDIX A; STABILITY OF AN INFINITE SET OF MATRICES 94 XI. APPENDIX B; ROSENBROCK'S OPTIMIZATION METHOD 96 XII. APPENDIX C: EXPANSION OF LYAPUNOV MATRIX EQUATION 98 XIII. APPENDIX D: COMPUTER PROGRAMS 100 1 I. INTRODUCTION It is well-known that many dynamical systems encountered in engineering and physical sciences can be modeled by systems of ordinary differential equations and that such differential equations are frequently nonlinear. For the engineers and scientists involved in modeling, anal­ ysis and design of such dynamical systems, stability is a fundamental problem. The concept of stability has its origin in mechanics where the position of equilibrium (rest) of a rigid body is considered to be stable, if it returns to its original position of equilibrium after a small dis­ turbance. The nonlinear differential equations representing the dynami­ cal system, in general, are so complex that they cannot be solved analytically in a closed form. Thus, in order to ascertain the qualita­ tive behavior of an equilibrium point of a dynamical system alternative methods of analysis are required. In 1892, A.M. Lyapunov, a Russian mathematician proposed two methods known as Indirect (First) method and Direct (Second) method to investigate the stability of dynamical systems represented by differential equations. Although Lyapunov's stability theory (see [1]) is playing an important role in modern control theory, his work went unnoticed for a long time. Subsequently, much work has been done on the extension and application of his work to systems represented by difference equations, stochastic dif­ ferential equations, functional differential equations, Volterra integro- differential equations, partial differential equations and hybrid systems 2 which are appropriately modeled by a mixture of different types of equations. Of particular importance is the Direct method, which has its origin in energy considerations, and through which one can ascertain the quali­ tative properties of the equilibrium of a dynamical system without any knowledge of its solution trajectories. In the analysis and design by Lyapunov's Direct method, the concept of asymptotic stability and the domain of attraction of an equilibrium is invaluable. In the literature, the domain of attraction is also referred to as the region of attraction or as the asymptotic stability region of an equilibrium. The domain of attraction of an equilibrium is a region with the equilibrium point in its interior and having the property that the trajectories of the system starting at any point within this region will eventually approach the equilibrium point. To determine an estimate for the domain of attraction of an equilibrium by the Lyapunov's Direct method, we need to find a scalar function such that this function and its time derivative along the solutions of the differential equation of the system in question satisfy certain conditions in some neighborhood of the given equilibrium point. (Without loss of generality, the equilibrium point will be assumed to be the origin of R^.) Although the Direct method of Lyapunov is a powerful tool available for the analysis and design of nonlinear dynamical systems, it suffers from several drawbacks. Notably, there is no universal and systematic method available which tells us how to find the required Lyapunov function. Although converse Lyapunov theorems have been estab­ lished, these results provide in general no clue (except in the case of 3 linear equations) as how to construct Lyapunov functions. In addition, finding a Lyapunov function successfully does not necessarily mean that it is necessarily the best choice in a particular problem. The prevail­ ing opinion among researchers is that even if applicable,it often requires excessive computation time to find a reasonably satisfactory Lyapunov function. Generally, the degree of the above difficulties associated with the Lyapunov theory increases as a system becomes large and complex. For this reason, to analyze the qualitative behavior of large-scale dynamical systems, it is frequently convenient to view such systems as interconnected systems composed of several lower order free subsystems. The analysis of such large-scale systems can often be accomplished in terms of the prop­ erties of the simpler subsystems and in terms of the properties of the interconnecting structure. This dissertation is devoted to the development of systematic, efficient and fast algoritlims to estimate the domain of attraction of general and large-scale nonlinear dynamical systems. 4 II. NOTATION The symbol i denotes Y-1. Let U and V be arbitrary sets. If u is an element of U we write u e U. If U is a subset of V, we write UC V and we denote the boundary of U by 3U. If W is a convex polyhedral region, then the elements of the set E(W) denotes its extreme vertices and K[W] = WU9W denotes its convex hull.
Load more

Recommended publications
  • Solution Bounds, Stability and Attractors' Estimates of Some Nonlinear Time-Varying Systems
    1 Solution Bounds, Stability and Attractors’ Estimates of Some Nonlinear Time-Varying Systems Mark A. Pinsky and Steve Koblik Abstract. Estimation of solution norms and stability for time-dependent nonlinear systems is ubiquitous in numerous applied and control problems. Yet, practically valuable results are rare in this area. This paper develops a novel approach, which bounds the solution norms, derives the corresponding stability criteria, and estimates the trapping/stability regions for a broad class of the corresponding systems. Our inferences rest on deriving a scalar differential inequality for the norms of solutions to the initial systems. Utility of the Lipschitz inequality linearizes the associated auxiliary differential equation and yields both the upper bounds for the norms of solutions and the relevant stability criteria. To refine these inferences, we introduce a nonlinear extension of the Lipschitz inequality, which improves the developed bounds and estimates the stability basins and trapping regions for the corresponding systems. Finally, we conform the theoretical results in representative simulations. Key Words. Comparison principle, Lipschitz condition, stability criteria, trapping/stability regions, solution bounds AMS subject classification. 34A34, 34C11, 34C29, 34C41, 34D08, 34D10, 34D20, 34D45 1. INTRODUCTION. We are going to study a system defined by the equation n (1) xAtxftxFttt , , [0 , ), x , ft ,0 0 where matrix A nn and functions ft:[ , ) nn and F : n are continuous and bounded, and At is also continuously differentiable. It is assumed that the solution, x t, x0 , to the initial value problem, x t0, x 0 x 0 , is uniquely defined for tt0 . Note that the pertained conditions can be found, e.g., in [1] and [2].
    [Show full text]
  • Strange Attractors and Classical Stability Theory
    Nonlinear Dynamics and Systems Theory, 8 (1) (2008) 49–96 Strange Attractors and Classical Stability Theory G. Leonov ∗ St. Petersburg State University Universitetskaya av., 28, Petrodvorets, 198504 St.Petersburg, Russia Received: November 16, 2006; Revised: December 15, 2007 Abstract: Definitions of global attractor, B-attractor and weak attractor are introduced. Relationships between Lyapunov stability, Poincare stability and Zhukovsky stability are considered. Perron effects are discussed. Stability and instability criteria by the first approximation are obtained. Lyapunov direct method in dimension theory is introduced. For the Lorenz system necessary and sufficient conditions of existence of homoclinic trajectories are obtained. Keywords: Attractor, instability, Lyapunov exponent, stability, Poincar´esection, Hausdorff dimension, Lorenz system, homoclinic bifurcation. Mathematics Subject Classification (2000): 34C28, 34D45, 34D20. 1 Introduction In almost any solid survey or book on chaotic dynamics, one encounters notions from classical stability theory such as Lyapunov exponent and characteristic exponent. But the effect of sign inversion in the characteristic exponent during linearization is seldom mentioned. This effect was discovered by Oscar Perron [1], an outstanding German math- ematician. The present survey sets forth Perron’s results and their further development, see [2]–[4]. It is shown that Perron effects may occur on the boundaries of a flow of solutions that is stable by the first approximation. Inside the flow, stability is completely determined by the negativeness of the characteristic exponents of linearized systems. It is often said that the defining property of strange attractors is the sensitivity of their trajectories with respect to the initial data. But how is this property connected with the classical notions of instability? For continuous systems, it was necessary to remember the almost forgotten notion of Zhukovsky instability.
    [Show full text]
  • Chapter 8 Stability Theory
    Chapter 8 Stability theory We discuss properties of solutions of a first order two dimensional system, and stability theory for a special class of linear systems. We denote the independent variable by ‘t’ in place of ‘x’, and x,y denote dependent variables. Let I ⊆ R be an interval, and Ω ⊆ R2 be a domain. Let us consider the system dx = F (t, x, y), dt (8.1) dy = G(t, x, y), dt where the functions are defined on I × Ω, and are locally Lipschitz w.r.t. variable (x, y) ∈ Ω. Definition 8.1 (Autonomous system) A system of ODE having the form (8.1) is called an autonomous system if the functions F (t, x, y) and G(t, x, y) are constant w.r.t. variable t. That is, dx = F (x, y), dt (8.2) dy = G(x, y), dt Definition 8.2 A point (x0, y0) ∈ Ω is said to be a critical point of the autonomous system (8.2) if F (x0, y0) = G(x0, y0) = 0. (8.3) A critical point is also called an equilibrium point, a rest point. Definition 8.3 Let (x(t), y(t)) be a solution of a two-dimensional (planar) autonomous system (8.2). The trace of (x(t), y(t)) as t varies is a curve in the plane. This curve is called trajectory. Remark 8.4 (On solutions of autonomous systems) (i) Two different solutions may represent the same trajectory. For, (1) If (x1(t), y1(t)) defined on an interval J is a solution of the autonomous system (8.2), then the pair of functions (x2(t), y2(t)) defined by (x2(t), y2(t)) := (x1(t − s), y1(t − s)), for t ∈ s + J (8.4) is a solution on interval s + J, for every arbitrary but fixed s ∈ R.
    [Show full text]
  • Robot Dynamics and Control Lecture 8: Basic Lyapunov Stability Theory
    MCE/EEC 647/747: Robot Dynamics and Control Lecture 8: Basic Lyapunov Stability Theory Reading: SHV Appendix Mechanical Engineering Hanz Richter, PhD MCE503 – p.1/17 Stability in the sense of Lyapunov A dynamic system x˙ = f(x) is Lyapunov stable or internally stable about an equilibrium point xeq if state trajectories are confined to a bounded region whenever the initial condition x0 is chosen sufficiently close to xeq. Mathematically, given R> 0 there always exists r > 0 so that if ||x0 − xeq|| <r, then ||x(t) − xeq|| <R for all t> 0. As seen in the figure R defines a desired confinement region, while r defines the neighborhood of xeq where x0 must belong so that x(t) does not exit the confinement region. R r xeq x0 x(t) MCE503 – p.2/17 Stability in the sense of Lyapunov... Note: Lyapunov stability does not require ||x(t)|| to converge to ||xeq||. The stronger definition of asymptotic stability requires that ||x(t)|| → ||xeq|| as t →∞. Input-Output stability (BIBO) does not imply Lyapunov stability. The system can be BIBO stable but have unbounded states that do not cause the output to be unbounded (for example take x1(t) →∞, with y = Cx = [01]x). The definition is difficult to use to test the stability of a given system. Instead, we use Lyapunov’s stability theorem, also called Lyapunov’s direct method. This theorem is only a sufficient condition, however. When the test fails, the results are inconclusive. It’s still the best tool available to evaluate and ensure the stability of nonlinear systems.
    [Show full text]
  • Analysis of ODE Models
    Analysis of ODE Models P. Howard Fall 2009 Contents 1 Overview 1 2 Stability 2 2.1 ThePhasePlane ................................. 5 2.2 Linearization ................................... 10 2.3 LinearizationandtheJacobianMatrix . ...... 15 2.4 BriefReviewofLinearAlgebra . ... 20 2.5 Solving Linear First-Order Systems . ...... 23 2.6 StabilityandEigenvalues . ... 28 2.7 LinearStabilitywithMATLAB . .. 35 2.8 Application to Maximum Sustainable Yield . ....... 37 2.9 Nonlinear Stability Theorems . .... 38 2.10 Solving ODE Systems with matrix exponentiation . ......... 40 2.11 Taylor’s Formula for Functions of Multiple Variables . ............ 44 2.12 ProofofPart1ofPoincare–Perron . ..... 45 3 Uniqueness Theory 47 4 Existence Theory 50 1 Overview In these notes we consider the three main aspects of ODE analysis: (1) existence theory, (2) uniqueness theory, and (3) stability theory. In our study of existence theory we ask the most basic question: are the ODE we write down guaranteed to have solutions? Since in practice we solve most ODE numerically, it’s possible that if there is no theoretical solution the numerical values given will have no genuine relation with the physical system we want to analyze. In our study of uniqueness theory we assume a solution exists and ask if it is the only possible solution. If we are solving an ODE numerically we will only get one solution, and if solutions are not unique it may not be the physically interesting solution. While it’s standard in advanced ODE courses to study existence and uniqueness first and stability 1 later, we will start with stability in these note, because it’s the one most directly linked with the modeling process.
    [Show full text]
  • Combinatorial and Analytical Problems for Fractals and Their Graph Approximations
    UPPSALA DISSERTATIONS IN MATHEMATICS 112 Combinatorial and analytical problems for fractals and their graph approximations Konstantinos Tsougkas Department of Mathematics Uppsala University UPPSALA 2019 Dissertation presented at Uppsala University to be publicly examined in Polhemsalen, Ångströmlaboratoriet, Lägerhyddsvägen 1, Uppsala, Friday, 15 February 2019 at 13:15 for the degree of Doctor of Philosophy. The examination will be conducted in English. Faculty examiner: Professor Ben Hambly (Mathematical Institute, University of Oxford). Abstract Tsougkas, K. 2019. Combinatorial and analytical problems for fractals and their graph approximations. Uppsala Dissertations in Mathematics 112. 37 pp. Uppsala: Department of Mathematics. ISBN 978-91-506-2739-8. The recent field of analysis on fractals has been studied under a probabilistic and analytic point of view. In this present work, we will focus on the analytic part developed by Kigami. The fractals we will be studying are finitely ramified self-similar sets, with emphasis on the post-critically finite ones. A prototype of the theory is the Sierpinski gasket. We can approximate the finitely ramified self-similar sets via a sequence of approximating graphs which allows us to use notions from discrete mathematics such as the combinatorial and probabilistic graph Laplacian on finite graphs. Through that approach or via Dirichlet forms, we can define the Laplace operator on the continuous fractal object itself via either a weak definition or as a renormalized limit of the discrete graph Laplacians on the graphs. The aim of this present work is to study the graphs approximating the fractal and determine connections between the Laplace operator on the discrete graphs and the continuous object, the fractal itself.
    [Show full text]
  • Stability Theory for Ordinary Differential Equations 1. Introduction and Preliminaries
    JOURNAL OF THE CHUNGCHEONG MATHEMATICAL SOCIETY Volume 1, June 1988 Stability Theory for Ordinary Differential Equations Sung Kyu Choi, Keon-Hee Lee and Hi Jun Oh ABSTRACT. For a given autonomous system xf = /(a?), we obtain some properties on the location of positive limit sets and investigate some stability concepts which are based upon the existence of Liapunov functions. 1. Introduction and Preliminaries The classical theorem of Liapunov on stability of the origin 鉛 = 0 for a given autonomous system xf = makes use of an auxiliary function V(.x) which has to be positive definite. Also, the time deriva­ tive V'(⑦) of this function, as computed along the solution, has to be negative definite. It is our aim to investigate some stability concepts of solutions for a given autonomous system which are based upon the existence of suitable Liapunov functions. Let U C Rn be an open subset containing 0 G Rn. Consider the autonomous system x' = /(⑦), where xf is the time derivative of the function :r(t), defined by the continuous function f : U — Rn. When / is C1, to every point t()in R and Xq in 17, there corresponds the unique solution xq) of xf = f(x) such that ^(to) = ⑦⑴ For such a solution, let us denote I(xq) = (aq) the interval where it is defined (a, ⑵ may be infinity). Let f : (a, &) -나 R be a continuous function. Then f is decreasing on (a, b) if and only if the upper right-sided Dini derivative D+f(t) = lim sup f〔t + h(-f(t) < o 九 一>o+ h Received by the editors on March 25, 1988.
    [Show full text]
  • Stability and Bifurcation of Dynamical Systems
    STABILITY AND BIFURCATION OF DYNAMICAL SYSTEMS Scope: • To remind basic notions of Dynamical Systems and Stability Theory; • To introduce fundaments of Bifurcation Theory, and establish a link with Stability Theory; • To give an outline of the Center Manifold Method and Normal Form theory. 1 Outline: 1. General definitions 2. Fundaments of Stability Theory 3. Fundaments of Bifurcation Theory 4. Multiple bifurcations from a known path 5. The Center Manifold Method (CMM) 6. The Normal Form Theory (NFT) 2 1. GENERAL DEFINITIONS We give general definitions for a N-dimensional autonomous systems. ••• Equations of motion: x(t )= Fx ( ( t )), x ∈ »N where x are state-variables , { x} the state-space , and F the vector field . ••• Orbits: Let xS (t ) be the solution to equations which satisfies prescribed initial conditions: x S(t )= F ( x S ( t )) 0 xS (0) = x The set of all the values assumed by xS (t ) for t > 0is called an orbit of the dynamical system. Geometrically, an orbit is a curve in the phase-space, originating from x0. The set of all orbits is the phase-portrait or phase-flow . 3 ••• Classifications of orbits: Orbits are classified according to their time-behavior. Equilibrium (or fixed -) point : it is an orbit xS (t ) =: xE independent of time (represented by a point in the phase-space); Periodic orbit : it is an orbit xS (t ) =:xP (t ) such that xP(t+ T ) = x P () t , with T the period (it is a closed curve, called cycle ); Quasi-periodic orbit : it is an orbit xS (t ) =:xQ (t ) such that, given an arbitrary small ε > 0 , there exists a time τ for which xQ(t+τ ) − x Q () t ≤ ε holds for any t; (it is a curve that densely fills a ‘tubular’ space); Non-periodic orbit : orbit xS (t ) with no special properties.
    [Show full text]
  • Arnold: Swimming Against the Tide / Boris Khesin, Serge Tabachnikov, Editors
    ARNOLD: Real Analysis A Comprehensive Course in Analysis, Part 1 Barry Simon Boris A. Khesin Serge L. Tabachnikov Editors http://dx.doi.org/10.1090/mbk/086 ARNOLD: AMERICAN MATHEMATICAL SOCIETY Photograph courtesy of Svetlana Tretyakova Photograph courtesy of Svetlana Vladimir Igorevich Arnold June 12, 1937–June 3, 2010 ARNOLD: Boris A. Khesin Serge L. Tabachnikov Editors AMERICAN MATHEMATICAL SOCIETY Providence, Rhode Island Translation of Chapter 7 “About Vladimir Abramovich Rokhlin” and Chapter 21 “Several Thoughts About Arnold” provided by Valentina Altman. 2010 Mathematics Subject Classification. Primary 01A65; Secondary 01A70, 01A75. For additional information and updates on this book, visit www.ams.org/bookpages/mbk-86 Library of Congress Cataloging-in-Publication Data Arnold: swimming against the tide / Boris Khesin, Serge Tabachnikov, editors. pages cm. ISBN 978-1-4704-1699-7 (alk. paper) 1. Arnold, V. I. (Vladimir Igorevich), 1937–2010. 2. Mathematicians–Russia–Biography. 3. Mathematicians–Soviet Union–Biography. 4. Mathematical analysis. 5. Differential equations. I. Khesin, Boris A. II. Tabachnikov, Serge. QA8.6.A76 2014 510.92–dc23 2014021165 [B] Copying and reprinting. Individual readers of this publication, and nonprofit libraries acting for them, are permitted to make fair use of the material, such as to copy select pages for use in teaching or research. Permission is granted to quote brief passages from this publication in reviews, provided the customary acknowledgment of the source is given. Republication, systematic copying, or multiple reproduction of any material in this publication is permitted only under license from the American Mathematical Society. Permissions to reuse portions of AMS publication content are now being handled by Copyright Clearance Center’s RightsLink service.
    [Show full text]
  • An Introduction to Dynamical Systems and Chaos G.C
    An Introduction to Dynamical Systems and Chaos G.C. Layek An Introduction to Dynamical Systems and Chaos 123 G.C. Layek Department of Mathematics The University of Burdwan Burdwan, West Bengal India ISBN 978-81-322-2555-3 ISBN 978-81-322-2556-0 (eBook) DOI 10.1007/978-81-322-2556-0 Library of Congress Control Number: 2015955882 Springer New Delhi Heidelberg New York Dordrecht London © Springer India 2015 This work is subject to copyright. All rights are reserved by the Publisher, whether the whole or part of the material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation, broadcasting, reproduction on microfilms or in any other physical way, and transmission or information storage and retrieval, electronic adaptation, computer software, or by similar or dissimilar methodology now known or hereafter developed. The use of general descriptive names, registered names, trademarks, service marks, etc. in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant protective laws and regulations and therefore free for general use. The publisher, the authors and the editors are safe to assume that the advice and information in this book are believed to be true and accurate at the date of publication. Neither the publisher nor the authors or the editors give a warranty, express or implied, with respect to the material contained herein or for any errors or omissions that may have been made. Printed on acid-free paper Springer (India) Pvt. Ltd. is part of Springer Science+Business Media (www.springer.com) Dedicated to my father Late Bijoychand Layek for his great interest in my education.
    [Show full text]
  • The Fractional View of Complexity
    entropy Editorial The Fractional View of Complexity António M. Lopes 1,∗ and J.A. Tenreiro Machado 2 1 UISPA–LAETA/INEGI, Faculty of Engineering, University of Porto, R. Dr. Roberto Frias, 4200-465 Porto, Portugal 2 Institute of Engineering, Polytechnic of Porto, Deptartment of Electrical Engineering, R. Dr. António Bernardino de Almeida, 431, 4249-015 Porto, Portugal; [email protected] * Correspondence: [email protected]; Tel.: +351-220413486 Received: 27 November 2019; Accepted: 11 December 2019; Published: 13 December 2019 Keywords: fractals; fractional calculus; complex systems; dynamics; entropy; information theory Fractal analysis and fractional differential equations have been proven as useful tools for describing the dynamics of complex phenomena characterized by long memory and spatial heterogeneity. There is a general agreement about the relation between the two perspectives, but the formal mathematical arguments supporting their relation are still being developed. The fractional derivative of real order appears as the degree of structural heterogeneity between homogeneous and inhomogeneous domains. A purely real derivative order would imply a system with no characteristic scale, where a given property would hold regardless of the scale of the observations. However, in real-world systems, physical cut-offs may prevent the invariance spreading over all scales and, therefore, complex-order derivatives could yield more realistic models. Information theory addresses the quantification and communication of information. Entropy and complexity are concepts that often emerge in relation to systems composed of many elements that interact with each other, which appear intrinsically difficult to model. This Special Issue focuses on the synergies of fractals or fractional calculus and information theory tools, such as entropy, when modeling complex phenomena in engineering, physics, life, and social sciences.
    [Show full text]
  • Linear Hydrodynamic Stability
    COMMUNICATION Linear Hydrodynamic Stability Y. Charles Li Communicated by Christina Sormani Introduction Hydrodynamic instability and turbulence are ubiquitous in nature, such as the air flow around an airplane of Figure 1. Turbulence was also the subject of paintings by Leonardo da Vinci and Vincent van Gogh (Figure 2). Tur- bulence is the last unsolved problem of classical physics. Mathematically, turbulence is governed by the Navier– Stokes equations, for which even the basic question of well-posedness is not completely solved. Indeed, the global well-posedness of the 3D Navier–Stokes equations is one of the seven Clay millennium prize problems [1]. Hydrodynamic stability goes back to such luminaries as Helmholtz, Kelvin, Rayleigh, O. Reynolds, A. Sommerfeld, Heisenberg, and G. I. Taylor. Many treatises have been written on the subject [5]. Linear hydrodynamic stability theory applies the sim- ple idea of linear approximation of a function through its tangent to function spaces. Hydrodynamicists have been Figure 1. Hydrodynamic instability and turbulence trying to lay down a rigorous mathematical foundation are ubiquitous in nature, such as the turbulent vortex for linear hydrodynamic stability theory ever since its air flow around the tip of an airplane wing. beginning [5]. Recent results on the solution operators of Euler and Navier–Stokes equations [2] [3] [4] imply that the simple idea of tangent line approximation does not apply because the derivative does not exist in the inviscid Linear Approximation in the Simplest Setting case, thus the linear Euler equations fail to provide a linear Let us start with a real-valued function of one variable approximation to inviscid hydrodynamic stability.
    [Show full text]