Thermodynamics of Chaotic Systems
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Keynote Presentations at TSAPS Meeting 2020, Nov. 12-14, UTA
Keynote Presentations at TSAPS Meeting 2020, Nov. 12-14, UTA Fractal Universality in Nature Boltzmann Medal of the International Union of Pure & Applied Physics (2013). His research concerns instability, chaos, pattern formation, Diverse phenomena often yield unexpected and turbulence in fluid flows, granular media, similarities. In the 17th century Newton thought chemical systems, and swimming bacteria. He about the gravitational force between the earth and his students and collaborators have and an apple falling from a tree, and he said “I observed, developed, or discovered the began to think of gravity extending to the orb of transition to chaos in fluids in several different the Moon.” Systems of many particles (atoms, geometries, a laboratory model of Jupiter's molecules, or macroscopic grains) can similarly Great Red Spot, localized structures exhibit universal behavior. For example, studies ("oscillons") in oscillating granular media, of phase transitions in the 20th century methods for characterizing chaos, "Turing" culminated in Kenneth Wilson’s theory of patterns in reaction-diffusion systems, and universality in transitions in the phase of anomalous diffusion and Lévy flights in systems as different as fluids and magnets, for geophysical flows. His papers have been cited which Wilson was awarded the Nobel Prize in more than 45000 times (Google Scholar). 1982. The present talk examines spatial patterns that emerge in systems driven away from thermodynamic equilibrium by imposed gradients (e.g., in pressure, temperature, nutrient concentration). Experiments, observations of natural phenomena, and mathematical models are providing insights into the formation of ordered patterns in physical, chemical, and biological systems, as will be illustrated through examples that exhibit remarkable mathematical similarity, such as the wrinkling of the edge of dendrites, some flowers, torn plastic sheets, and bacterial colonies. -
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. -
Chaos Theory and Its Application in the Atmosphere
Chaos Theory and its Application in the Atmosphere by XubinZeng Department of Atmospheric Science Colorado State University Fort Collins, Colorado Roger A. Pielke, P.I. NSF Grant #ATM-8915265 CHAOS THEORY AND ITS APPLICATION IN THE ATMOSPHERE Xubin Zeng Department of Atmospheric Science CoJorado State University Fort Collins, Colorado Summer, 1992 Atmospheric Science Paper No. 504 \llIlll~lIl1ll~I""I1~II~'I\1 U16400 7029194 ABSTRACT CHAOS THEORY AND ITS APPLICATION IN THE ATMOSPHERE Chaos theory is thoroughly reviewed, which includes the bifurcation and routes to tur bulence, and the characterization of chaos such as dimension, Lyapunov exponent, and Kolmogorov-Sinai entropy. A new method is developed to compute Lyapunov exponents from limited experimental data. Our method is tested on a variety of known model systems, and it is found that our algorithm can be used to obtain a reasonable Lyapunov exponent spectrum from only 5000 data points with a precision of 10-1 or 10-2 in 3- or 4-dimensional phase space, or 10,000 data points in 5-dimensional phase space. On 1:he basis of both the objective analyses of different methods for computing the Lyapunov exponents and our own experience, which is subjective, this is recommended as a good practical method for estiIpating the Lyapunov-exponent spectrum from short time series of low precision. The application of chaos is divided into three categories: observational data analysis, llew ideas or physical insights inspired by chaos, and numerical model output analysis. Corresponding with these categories, three subjects are studied. First, the fractal dimen sion, Lyapunov-exponent spectrum, Kolmogorov entropy, and predictability are evaluated from the observed time series of daily surface temperature and pressure over several regions of the United States and the North Atlantic Ocean with different climatic signal-to-noise ratios. -
Lecture 11: Feigenbaum's Analysis of Period Doubling, Superstability of Fixed Points and Period-P Points, Renor- Malisation, U
Lecture notes #11 Nonlinear Dynamics YFX1520 Lecture 11: Feigenbaum’s analysis of period doubling, superstability of fixed points and period-p points, renor- malisation, universal limiting function, discrete time dy- namics analysis methods, Poincaré section, Poincaré map, Lorenz section, attractor reconstruction Contents 1 Feigenbaum’s analysis of period doubling 2 1.1 Feigenbaum constants . .2 1.2 Superstable fixed points and period-p points . .2 1.3 Renormalisation and the Feigenbaum constants . .5 1.4 Numerical determination of the Feigenbaum α constant . .7 2 Discrete time analysis methods 8 2.1 Poincaré section and Poincaré map . .9 2.1.1 Example of finding a Poincaré map formula . .9 2.2 Poincaré analysis of the periodically driven damped Duffing oscillator . 11 2.3 Poincaré analysis of the Rössler attractor . 13 3 Lorenz section of 3-D attractor 15 4 Attractor reconstruction 16 D. Kartofelev 1/16 K As of March 10, 2021 Lecture notes #11 Nonlinear Dynamics YFX1520 1 Feigenbaum’s analysis of period doubling In this lecture we are continuing our study of one-dimensional maps as simplified models of chaos and as tools for analysing higher order differential equations. We have already encountered maps in this role. The Lorenz map provided strong evidence that the Lorenz attractor is truly strange, and is not just a long- period limit-cycle, see Lectures 9 and 10. 1.1 Feigenbaum constants The Feigenbaum constants were presented during Lecture 10. Slide: 3 1-D unimodal maps and Feigenbaum constants ∆n 1 rn 1 rn 2 δ = lim − = lim − − − 4.669201609... (1) n ∆n n rn rn 1 ≈ →∞ →∞ − − dn 1 α = lim − 2.502907875.. -
Foundations of the Scale-Symmetric Physics
Copyright © 2015 by Sylwester Kornowski All rights reserved Foundations of the Scale-Symmetric Physics (Main Article No 3: Chaos Theory) Sylwester Kornowski Abstract: Here, applying the Scale-Symmetric Theory (SST), we show how particle physics via the Chaos Theory leads to the cosmological dark-matter structures and mental solitons. Moreover, the interactions of the cosmological dark-matter structures with baryonic matter via weak interactions of leptons, lead to the untypical motions of stars in galaxies and to other cosmological structures such as AGN composed of a torus and a central- condensate/modified-black-hole or solar system. Most important in the Chaos Theory (ChT) is to understand physical meaning of a logistic map for the baryons - it concerns the black- body spectrum and the ratio of the masses of charged kaon and pion. Such logistic map leads to the first Feigenbaum constant related to the period-doubling bifurcations that in a limit lead to the onset of chaos. In the period-doubling bifurcations for proton there appear the orbits of period-4 and higher periods. We show that the orbits of period-4 follow from the structure of baryons and that they lead to the Titius-Bode law for the nuclear strong interactions. Calculated here on base of the structure of proton the first Feigenbaum constant is 4.6692033 and it is close to the mathematical value 4.6692016… Contents 1. Introduction 86 2. The logistic map for proton, physical origin of the period-doubling cascade In proton and the Feigenbaum constants, and the leaking dark-matter structures 87 2.1 The logistic map for proton 87 2.2 The Titius-Bode law for the nuclear strong interactions as a result of creation of attractors in the logistic map for proton 88 2.3 Physical origin of the period-doubling cascade for proton and Feigenbaum constants 90 2.4 The leaking dark-matter structures 90 2.5 The Titius-Bode law and bifurcation 90 2.6 Prime numbers and the Titius-Bode law and solar system 91 3. -
Theoretical-Heuristic Derivation Sommerfeld's Fine Structure
Theoretical-heuristic derivation Sommerfeld’s fine structure constant by Feigenbaum’s constant (delta): perodic logistic maps of double bifurcation Angel Garcés Doz [email protected] Abstract In an article recently published in Vixra: http://vixra.org/abs/1704.0365. Its author (Mario Hieb) conjectured the possible relationship of Feigen- baum’s constant delta with the fine-structure constant of electromag- netism (Sommerfeld’s Fine-Structure Constant). In this article it demon- strated, that indeed, there is an unequivocal physical-mathematical rela- tionship. The logistic map of double bifurcation is a physical image of the random process of the creation-annihilation of virtual pairs lepton- antilepton with electric charge; Using virtual photons. The probability of emission or absorption of a photon by an electron is precisely the fine structure constant for zero momentum, that is to say: Sommerfeld’s Fine- Structure Constant. This probability is coded as the surface of a sphere, or equivalently: four times the surface of a circle. The original, conjectured calculation of Mario Hieb is corrected or improved by the contribution of the entropies of the virtual pairs of leptons with electric charge: muon, tau and electron. Including a correction factor due to the contributions of virtual bosons W and Z; And its decay in electrically charged leptons and quarks. Introduction The main geometric-mathematical characteristics of the logistic map of double universal bifurcation, which determines the two Feigenbaum’s constants; they are: 1) The first Feigenbaum constant is the limiting ratio of each bifurcation interval to the next between every period doubling, of a one-parameter map. -
PY2T20: CHAOS and COMPLEXITY (12 Lectures) Stefan Hutzler
PY2T20: CHAOS AND COMPLEXITY (12 lectures) Stefan Hutzler lecture notes at: http://www.tcd.ie/Physics/Foams/Lecture Notes/PY2T20ChaosAndComplexity February 7, 2014 Contents 1 A glossary 1 2 Examples of non-linear and chaotic behaviour 3 2.1 Population dynamics . 3 2.2 Non-linear electrical circuit . 6 2.3 Lorenz model of atmospheric convection . 7 2.4 Summary of observations . 7 3 Universal properties and self-similarity 8 3.1 Feigenbaum constants . 8 3.2 Measuring chaos . 9 3.3 Universality of chaos . 10 4 Determinism 12 5 Dynamics in phase space: Motion of the pendulum 13 5.1 Equation of motion for damped driven pendulum . 13 5.2 Phase space . 15 5.3 Damped driven pendulum: period doubling and chaos . 17 5.4 Properties of trajectories . 17 6 Some theory of chaotic dynamics 19 6.1 Long-term behaviour of dissipative systems . 19 6.2 Stability of fixed points . 20 6.2.1 one dimension . 20 6.2.2 two dimensions . 21 6.2.3 three dimensions . 23 6.3 Analysis of limit cycles . 23 i 6.4 Examples for damped driven pendulum . 23 6.5 Quasi-periodicity . 24 6.6 Different routes to chaos . 24 7 Iterated maps 26 7.1 Motivation . 26 7.2 Bernoulli shift . 26 8 Fractals 29 8.1 A mathematical monster: the Koch curve . 29 8.2 Fractal dimensions . 30 8.3 Examples of fractals . 30 9 Strange attractors 32 9.1 Definition . 32 9.2 Baker’s transformation . 33 9.3 Stretching and folding for the logistic map . 33 10 Advanced topics 35 10.1 Hamiltonian systems (motivation) . -
Frequently Asked Questions About Nonlinear Science J.D
Frequently Asked Questions about Nonlinear Science J.D. Meiss Sept 2003 [1] About Sci.nonlinear FAQ This is version 2.0 (Sept. 2003) of the Frequently Asked Questions document for the newsgroup s ci.nonlinear. This document can also be found in Html format from: http://amath.colorado.edu/faculty/jdm/faq.html Colorado, http://www-chaos.engr.utk.edu/faq.html Tennessee, http://www.fen.bris.ac.uk/engmaths/research/nonlinear/faq.html England, http://www.sci.usq.edu.au/mirror/sci.nonlinear.faq/faq.html Australia, http://www.faqs.org/faqs/sci/nonlinear-faq/ Hypertext FAQ Archive Or in other formats: http://amath.colorado.edu/pub/dynamics/papers/sci.nonlinearFAQ.pdf PDF Format, http://amath.colorado.edu/pub/dynamics/papers/sci.nonlinearFAQ.rtf RTF Format, http://amath.colorado.edu/pub/dynamics/papers/sci.nonlinearFAQ.tex old version in TeX, http://www.faqs.org/ftp/faqs/sci/nonlinear-faq the FAQ's site, text version ftp://rtfm.mit.edu/pub/usenet/news.answers/sci/nonlinear-faq text format. This FAQ is maintained by Jim Meiss [email protected]. Copyright (c) 1995-2003 by James D. Meiss, all rights reserved. This FAQ may be posted to any USENET newsgroup, on-line service, or BBS as long as it is posted in its entirety and includes this copyright statement. This FAQ may not be distributed for financial gain. This FAQ may not be in cluded in commercial collections or compilations without express permission from the author. [1.1] What's New? Fixed lots of broken and outdated links. A few sites seem to be gone, and some new sites appeare d. -
Fall 2012 Cover.Indd 1 10/15/12 3:08 PM FALL 2012 Contents VOLUME 19 • NUMBER 3
The Magazine of Rhodes College • Fall 2012 THE SCIENCES AT RHODES Past, Present and Future Fall 2012 cover.indd 1 10/15/12 3:08 PM FALL 2012 Contents VOLUME 19 • NUMBER 3 2 Campus News Briefs on campus happenings 5 The Sciences at Rhodes—Past, Present and Future Conversations with faculty, alumni and current students who majored in or are currently engaged in one of the six science disciplines Rhodes offers: 6 The Biochemists and Molecular Biologists Professor Terry Hill, Amanda Johnson Winters ’99, Ross 10 Hilliard ’07, Xiao Wang ’13 10 The Biologists Professor Gary Lindquester, Veronica Lawson Gunn ’91, Brian Wamhoff ’96, Anahita Rahimi-Saber ’13 14 The Chemists Professor Darlene Loprete, Sid Strickland ’68, Tony Capizzani ’95, Ashley Tufton ’13 18 The Environmental Scientists Professor Rosanna Cappellato, Cary Fowler ’71, Christopher Wilson ’95, Alix Matthews ’14 22 The Neuroscientists Professor Robert Strandburg, Jim Robertson ’53 and Jon Robertson ’68, Michael Long ’97, Piper Carroll ’13 14 26 The Physicists Professor Brent Hoffmeister, Harry Swinney ’61, Charles Robertson Jr. ’65, Lars Monia ’15 30 A Case for the Support of the Sciences at Rhodes The importance of strengthening the sciences in the 21st century 32 Alumni News Class Notes, In Memoriam The 2011-2012 Honor Roll of Donors On the Cover From left: Alix Matthews ’14, Ashley Tufton ’13, Piper Carroll ’13, Lars Monia ’15 and Xiao Wang ’13, fi ve of the six science majors featured in this issue, at the Lynx 26 sculpture in front of the Peyton Nalle Rhodes Tower, home of the Physics Department Photography by Justin Fox Burks Contents_Fall ’12.indd 1 10/15/12 3:05 PM is published three times a year by Rhodes College, 2000 N. -
WP-82-086.Pdf
NOT FOR QUOTATION WITHOUT PERMISSION OF THE AUTHOR CHAOS IN NONLINEAR DYNAMICS AND THE LOGISTIC SUBSTITUTION MODEL Bill Keepin September 1982 WP-82-86 Working Papers are interim reports on work of the International Institute for Applied Systems Analysis and have received only limited review. Views or opinions expressed herein do not necessarily repre- sent those of the Institute or of its National Member Organizations. INTERNATIONAL INSTITUTE FOR APPLIED SYSTEYS ANALYSIS A-2361 Laxenburg, Austria The Tower is as wide and spacious as the sky itself ... Arid within this Tower, spacious and exquisite Zy ornamented, there are also hundreds of thousands. .of towers, each one of which is as exquisitely ornamented as the main Tower itself and as spucious as the sZ:y. And all these towers, beyond caZcuZation in number, stand not at all in one another's way; each preserves its individual existence in perfect harmony with all the rest; there is nothing here that bars one tower being fused with all the others ind7~viduallyand coZlectively; there is a state of perfect intermingling and yet of perfect orderliness ... all is contained in one and each contains all. D.T. Suzuki (1968) PREFACE A rekindled appreciation of an old cliche has touched off a flurry of activity in the field of nonlinear dynamics lately. The truism that nonlinearities often lead to wild and exotic behavior has been known for a long time, but only recently has it been studied carefully, and the discoveries are startling and profound. The simplest equation illuminating these features is the logistic equation (in discrete form), which has a long history of application to growth phenomena in biology and popu- lation dynamics. -
1 Introduction 2 Wright's Conjecture on a Nonlinear Delay Differential
Research Statement Jonathan Jaquette December 2020 1 Introduction My research broadly focuses on dynamics and differential equations, and in particular bridging the gap between what can be proven mathematically and what can be computed numerically. For example, standard numerical methods can solve an initial value problem for an ODE and provide local error bounds at each step. However a global error bound on the final solution requires the cumulative error be quantified. This quickly becomes a nontrivial problem in chaotic systems, where arbitrarily close initial conditions will inevitably diverge, and the difficulties compound in partial differential equations where the phase space is infinite dimensional. To that end, validated numerics have been developed to keep track of all the sources of error inherent to numerical calculations. To bridge the gap between numerics and a computer assisted proof, a problem must be translated into a list of the conditions that the computer can check. Most famously used to solve the four color theorem [1], computer assisted proofs have been employed to great effect in dynamics, proving results such as the universality of the Feigenbaum constants [2] and Smale's 14th problem on the nature of the Lorenz attractor [3]. I am particularly interested in developing constructive methods to study invariant sets and their stability in infinite dimensional dynamical systems. Analytically, this involves proving the- orems with explicitly verifiable hypotheses (e.g. rather than assuming \there exists some > 0", concretely quantifying how small must be). Computationally, this involves variety of numerical techniques from fields such as dynamical systems, partial differential equations, global optimization, and algebraic topology. -
Introduction to Chaos and the Logistic Map CS523 Assignment One – Spring 2013 the University of New Mexico
Introduction to Chaos and the Logistic Map CS523 Assignment One – Spring 2013 The University of New Mexico Karl Stolleis John Ericksen [email protected] [email protected] Introduction The following report is an introduction to the concepts of the logistic map function and its application to complex systems and chaos theory. The initial equation for the logistic map is as follows : 2 P(t +1)=R (Pt −Pt /k) where the population P at a given time step t is used to calculate the population at the next time step P(t +1) in the sequence. The value R is the the birth rate of the population minus the death rate. The constant k is the “carrying capacity,” or the number of individual organisms, that the organism's environment can support. [1] With some algebraic maneuvering the equation can be rewritten in the form: P(t +1)=R Pt (1−Pt ) where the value P is now the population given as a percentage of the total carrying capacity. [1] We will use both equations in this paper to demonstrate various principles. The logistic map is used as a basic demonstration of a mathematical equation that, despite its simplicity, can give rise to chaotic behavior. Chaos, in this context, simply means that the values generated by the logistic map, at a given R-value, will become unpredictable. Unlike the common definition of chaos, the chaos described by dynamical systems is really unpredictability arising from a deterministic structure, such as a mathematical equation. [2] The logistic map also demonstrates a hallmark of chaotic systems, namely high sensitivity to initial conditions.