Stochastic Oscillations Motivated by the Noisy and Rhythmic Firing

Total Page:16

File Type:pdf, Size:1020Kb

Stochastic Oscillations Motivated by the Noisy and Rhythmic Firing Submitted by Irene Tubikanec Submitted at Department of Stochastics Supervisor Univ.-Prof.in Dr.in Stochastic Oscillations Evelyn Buckwar December 2016 Motivated by the Noisy and Rhythmic Firing Activity of Neurons Master Thesis to obtain the academic degree of Diplom-Ingenieurin in the Master’s Program Industriemathematik JOHANNES KEPLER UNIVERSITY LINZ Altenbergerstraße 69 4040 Linz, Osterreich¨ www.jku.at DVR 0093696 „Don’t worry dreams aren’t real. They’re just neurons firing randomly in your brain.“ Katherine Applegate Eidesstattliche Erklärung Ich erkläre an Eides statt, dass ich die vorliegende Masterarbeit selbstständig und ohne fremde Hilfe verfasst, andere als die angegebenen Quellen und Hilfsmittel nicht benutzt bzw. die wörtlich oder sinngemäß entnommenen Stellen als solche kenntlich gemacht habe. Die vorliegende Masterarbeit ist mit dem elektronisch übermittelten Textdokument identisch. Linz, 01. Dezember 2016 Irene Tubikanec, BSc BSc Abstract A human brain contains billions of neurons. These are extremely complex dynamical systems that are affected by intrinsic channel noise and extrinsic synaptic noise. Os- cillatory behaviour is a phenomena that arises in single neurons as well as in neuronal networks. Based on the noisy and rhythmic firing activity of nerve cells, the aimof this thesis is to provide an overview on the existing theory of stochastic oscillations. The main question is how oscillations can be defined mathematically in a stochastic setting. This work suggests two very different definitions of a stochastic oscillator according to certain well-known deterministic tools. The first one states that the solution of a specific two-dimensional stochastic differential equation is a stochastic oscillator if it has infinitely many simple zeros almost surely. The second definition of a stochastic oscillator corresponds to the concept of a random periodic solution that is based on the cocycle property. Two particular stochastic equations are introduced each satisfying one of these definitions. For this purpose, two detailed proofs onthe validity of the first and the second definition, respectively, are presented. A second topic addressed by this work is the stability of stochastic equations. The system energy carries information on how the trajectory propagates in the phase plane. Besides, Lyapunov exponents describe the asymptotic exponential growth of random dynamical systems. Finally, this work provides an application of the developed theory to specific standard oscillatory models as well as to the Van der Pol oscillator on which the FitzHugh- Nagumo neuron model is based. Sample path simulations of the stochastic equations are provided by the implementation of the Euler-Maruyama method in MATLAB. Furthermore, an exact simulation method applied to the stochastic harmonic oscillator equation is introduced. Zusammenfassung Das menschliche Gehirn umfasst Milliarden von Neuronen. Das sind hochkomplexe dynamische Systeme, die intrinsischem Kanal- und extrinsischem Synapsenrauschen unterliegen. Oszillierendes Verhalten tritt in einzelnen Zellen als auch in Netzwerken auf. Aufgrund der rhythmischen und zufälligen neuronalen Impulse, ist es Ziel dieser Arbeit einen Überblick der aktuellen Theorie stochastischer Oszillatoren zu geben. Das Hauptanliegen ist die Beantwortung der Frage wie Oszillatoren in einem stochastis- chen Rahmen mathematisch definiert werden können. In Anlehnung an determinis- tische Aussagen, betrachtet diese Arbeit zwei mögliche Definitionen. Bei der ersten Variante wird die Lösung einer zweidimensionalen stochastischen Differentialgleichung als Oszillator definiert, falls sie fast sicher unendlich viele einfache Nullstellen aufweist. Die zweite Definition entspricht dem Konzept einer periodischen Lösung und basiert auf der cocycle Eigenschaft. Es werden zwei Gleichungen vorgestellt, welche je eine der beiden stochastischen Definitionen erfüllen. Die entsprechenden Beweise werden detailliert präsentiert. Des Weiteren wird die Stabilität von stochastischen Systemen thematisiert. Die Sys- temenergie gibt Auskunft über die Entwicklung der Trajektorie im Phasenraum. Außer- dem beschreiben Lyapunov Exponenten das asymptotische exponentielle Wachstum von stochastischen dynamischen Systemen. Neben der Anwendung erarbeiteter Theorien auf Standardmodelle erfolgt eine Betrach- tung der Van der Pol Gleichung, die den Grundstein des bekannten FitzHugh-Nagumo Neuronenmodells bildet. Die Simulation von Beispielpfaden erfolgt mit der Imple- mentierung des Euler-Maruyama Verfahrens in MATLAB. Ergänzend wird eine exakte Simulationsmethode für den harmonischen Oszillator diskutiert. Acknowledgments I would like to express my deep gratitude to my supervisor Prof.in Evelyn Buckwar for the opportunity to write this thesis, for giving me the possibility to decide on topics and contents, for enabling me to participate on specific conferences and for her engagement throughout my whole work. I would also like to thank my colleague and best friend Bernadett Stadler for construc- tive discussions and for proofreading. Special thanks to my life partner Michaela Fehringer for her patience and for her mental assistance. Finally, I owe my deepest gratitude to my parents who supported me during my whole life and, in particular, during my studies. Especially, I would like to acknowledge my mother for respecting all of my decisions and for her long lasting blind trust. Contents 1 Introduction1 1.1 Problem Description . .1 1.2 Research Questions . .2 1.3 Structure of the Thesis . .2 2 Introduction to Neuroscience4 2.1 Single Neurons . .4 2.1.1 Components and Functionality . .4 2.1.2 Noise and Rhythmicity . .5 2.2 Single Neuron Models . .6 2.2.1 Hodgkin-Huxley Model . .6 2.2.1.1 Equivalent Electrical Circuit . .7 2.2.1.2 Types of Ion Channels . .8 2.2.2 FitzHugh-Nagumo Model . .9 2.2.3 Van der Pol Model . 10 3 Deterministic Oscillation Theory 12 3.1 Definition of a Deterministic Oscillator 1 . 12 3.2 Definition of a Deterministic Oscillator 2 . 13 3.2.1 Deterministic Flow Property . 13 3.2.2 Fixed Points and Periodic Solutions . 15 3.3 System Stability . 16 3.3.1 Stability of Fixed Points . 16 3.3.2 Stability of Limit Cycles . 19 4 Stochastic Oscillation Theory 21 4.1 Definition of a Stochastic Oscillator 1 . 23 4.1.1 Stochastic Harmonic Oscillator . 23 Contents viii 4.1.2 Theorem of Girsanov . 24 4.2 Definition of a Stochastic Oscillator 2 . 29 4.2.1 Stochastic Cocycle Property . 30 4.2.2 Random Fixed Points and Periodic Solutions . 34 4.3 System Stability . 38 4.3.1 System Energy . 38 4.3.2 Lyapunov Exponents . 39 5 Theory Application on Specific Models 43 5.1 Deterministic Applications . 43 5.1.1 Harmonic Oscillator . 43 5.1.2 Damped Harmonic Oscillator . 45 5.1.3 Van der Pol Oscillator . 47 5.1.4 Nonlinear Oscillator . 49 5.2 Stochastic Applications . 50 5.2.1 Stochastic Harmonic Oscillator . 51 5.2.2 Stochastic Damped Harmonic Oscillator . 57 5.2.3 Stochastic Van der Pol Oscillator . 59 5.2.4 Stochastic Nonlinear Oscillator . 62 6 Conclusion 71 6.1 Experiences . 71 6.2 Future Work . 72 Bibliography 76 Chapter 1 Introduction A human brain contains billions of extremely complex dynamical systems called neu- rons. By using mathematical models that capture their main dynamics, one tries to reconstruct the firing of single neurons as well as neuronal interactions. Understanding how the human brain is working, and especially how neurons manage their interactive communication, could contribute to the comprehension of specific mechanisms that lead to diseases such as Alzheimer’s, Parkinson’s or Epilepsy. 1.1 Problem Description Oscillatory activity arises at each level of neuronal systems. Many neurons fire action potentials repetitively. The mechanisms, inducing rhythmic firing, differ across each level of neural systems. Since oscillatory behaviour has been realised in diseases as well, understanding those mechanisms and being able to control them is an important medical problem [11]. Mathematics and especially stochastics offer central possibilities to make a contribution to this crucial topic. Neurons communicate with the use of electrical impulses that are called spikes or ac- tion potentials. These signals propagate along the filamentary extensions of neural cells by passing through ion channels that fluctuate rapidly between the open and closed state. For that reason, neurons are affected by intrinsic channel noise. Since nerve cells are surrounded by amounts of other neurons, extrinsic synaptic noise arises in Chapter 1 Introduction 2 this dynamical systems as well. To capture neuronal noise the application of stochastic differential equations (SDEs), which model time dependent phenomena that underlie random effects, is of essential importance. SDEs came into being in course of the twen- tieth century and have been build on a more solid ground by Itô [20] and Stratonovich [32] in the middle of that century. Many crucial developments, based on their work, have been achieved in recent decades. Therefore, this special type of equations is a very innovative mathematical tool that provides still many open possibilities for research. 1.2 Research Questions Based on the noisy and rhythmic firing activity of neurons, the aim of this thesis isto provide an overview on stochastic oscillation theory. This work mainly addresses the following questions: 1. How can oscillations be defined mathematically in a stochastic setting according to the well-known deterministic tools? 2. Which tools concerning the treatment of system stability
Recommended publications
  • Student Version an Interactive Illustration of the Van Der Pol Oscillator
    STUDENT VERSION AN INTERACTIVE ILLUSTRATION OF THE VAN DER POL OSCILLATOR Mark A. Lau Kwan Electrical Engineering University of Turabo Gurabo PUERTO RICO STATEMENT The purpose of this paper is to present an interactive spreadsheet application that allows the reader to investigate the Van der Pol oscillator. Through a number of suggested activities, the reader will gain a better understanding of the qualitative behavior of solutions as the parameters of the governing differential equation are varied. A Brief Description of the Van der Pol Oscillator The Van der Pol oscillator is described by the nonlinear, second-order ordinary differential equation x¨ + µ(x2 − 1)x _ + !2x = 0; (1) where µ and ! are positive parameters, and x (a function of time t) is the quantity of interest (e.g., position or voltage). The quantitiesx _ andx ¨ denote the first- and second-order derivative with respect to time t, respectively. This celebrated equation (1) is attributed to the Dutch electrical engineer Balthasar Van der Pol, who pioneered experimental investigations in nonlinear dynamics in the early days of radio and telecommunications. He proposed his equation in order to describe the nonlinear oscillations produced by self-sustained oscillating triode circuits [5]. His equation has been extensively studied and finds numerous applications in engineering, physics, biology, sociology, and economics. The Van der Pol equation (1) introduces a nonlinear damping term, namely µ(x2 − 1)x _. Unlike the familiar linearly damped harmonic oscillator, the presence of the nonlinear damping term can 2 Van der Pol Oscillator Figure 1. Main user interface of the Microsoft Excel spreadsheet for investigating the behavior of the Van der Pol oscillator.
    [Show full text]
  • Van Der Pol Meets LSTM
    bioRxiv preprint doi: https://doi.org/10.1101/330548; this version posted May 25, 2018. The copyright holder for this preprint (which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission. Learning Nonlinear Brain Dynamics: van der Pol Meets LSTM Germán Abrevaya Aleksandr Aravkin Departamento de Física, FCEyN Department of Applied Mathematics Universidad de Buenos Aires University of Washington & IFIBA, CONICET Seattle, WA Buenos Aires, Argentina [email protected] [email protected] Guillermo Cecchi Irina Rish Pablo Polosecki IBM Research IBM Research IBM Research Yorktown Heights, NY Yorktown Heights, NY Yorktown Heights, NY [email protected] [email protected] [email protected] Peng Zheng Silvina Ponce Dawson Department of Applied Mathematics Departamento de Física, FCEyN University of Washington Universidad de Buenos Aires Seattle, WA & IFIBA, CONICET [email protected] Buenos Aires, Argentina [email protected] Abstract Many real-world data sets, especially in biology, are produced by highly multivari- ate and nonlinear complex dynamical systems. In this paper, we focus on brain imaging data, including both calcium imaging and functional MRI data. Standard vector-autoregressive models are limited by their linearity assumptions, while nonlinear general-purpose, large-scale temporal models, such as LSTM networks, typically require large amounts of training data, not always readily available in biological applications; furthermore, such models have limited interpretability. We introduce here a novel approach for learning a nonlinear differential equation model aimed at capturing brain dynamics. Specifically, we propose a variable-projection optimization approach to estimate the parameters of the multivariate (coupled) van der Pol oscillator, and demonstrate that such a model can accurately repre- sent nonlinear dynamics of the brain data.
    [Show full text]
  • Arxiv:Cond-Mat/0212203V1
    A nonlinear dynamical model of human gait Bruce J. West1,2,3 and Nicola Scafetta.1,2 1 Pratt School of EE Department, Duke University, P.O. Box 90291, Durham, NC 27701. 2 Physics Department, Duke University, Durham, NC 27701. and 3 Mathematics Division, Army Research Office, Research Triangle Park, NC 27709. (Dated: September 27, 2018) We present a nonlinear stochastic model of the human gait control system in a variety of gait regimes. The stride interval time series in normal human gait is characterized by slightly multifractal fluctuations. The fractal nature of the fluctuations become more pronounced under both an increase and decrease in the average gait. Moreover, the long-range memory in these fluctuations is lost when the gait is keyed on a metronome. The human locomotion is controlled by a network of neurons capable of producing a correlated syncopated output. The central nervous system is coupled to the motocontrol system, and together they control the locomotion of the gait cycle itself. The metronomic gait is simulated by a forced nonlinear oscillator with a periodic external force associated with the conscious act of walking in a particular way. PACS numbers: 05.45.-a,87.18.Sn, 05.45.Df, 87.17.Nn I. INTRODUCTION neural firing activity. The dynamics of human gate may also be voluntarily forced, for example, by following the Walking is a complex process which we have only re- frequency of a metronome. We model the complex gait cently begun to understand through the application of system by assuming that the amplitude of the impulses of nonlinear data processing techniques [1, 2, 3, 4] to study the correlated firing neural centers regulate only the un- interval data.
    [Show full text]
  • Abdus Salam United Nations Educational, Scientific and Cuftura! XA0053813 Organization International Centre International Atomic Energy Agency for Theoretical Physics
    the abdus salam united nations educational, scientific and cuftura! XA0053813 organization international centre international atomic energy agency for theoretical physics HARMONIC OSCILLATIONS, CHAOS AND SYNCHRONIZATION IN SYSTEMS CONSISTING OF VAN DER POL OSCILLATOR COUPLED TO A LINEAR OSCILLATOR P. Woafo i 31-09 J IC/99/188 United Nations Educational Scientific and Cultural Organization and International Atomic Energy Agency THE ABDUS SALAM INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS HARMONIC OSCILLATIONS, CHAOS AND SYNCHRONIZATION IN SYSTEMS CONSISTING OF VAN DER POL OSCILLATOR COUPLED TO A LINEAR OSCILLATOR P. Woafo1 Laboratoire de Mecanique, Faculte des Sciences, Universite de Yaounde I, B.P. 812, Yaounde, Cameroon and The Abdus Salam International Centre for Theoretical Physics, Trieste, Italy. Abstract This paper deals with the dynamics of a model describing systems consisting of the classical Van der Pol oscillator coupled gyroscopically to a linear oscillator. Both the forced and autonomous cases are considered. Harmonic response is investigated along with its stability boundaries. Condition for quenching phenomena in the autonomous case is derived. Neimark bifurcation is observed and it is found that our model shows period doubling and period-m sudden transitions to chaos. Synchronization of two and more systems in their chaotic regime is presented. MIRAMARE - TRIESTE December 1999 'Regular Associate of the Abdus Salam ICTP. I- Introduction Due to their occurrence in various scientific fields, ranging from biology, chemistry, physics to engineering, coupled nonlinear oscillators have been a subject of particular interest in recent years [1,2,3]. Among these coupled systems, a particular class is that containing self-sustained components such as the classical Van der Pol oscillator.
    [Show full text]
  • Hopf Bifurcation and Stability of Periodic Solutions for Van Der Pol
    Nonlinear Analysis 62 (2005) 141–165 www.elsevier.com/locate/na Hopf bifurcation and stability of periodic solutions for van der Pol equation with time delayଁ WenwuYu, Jinde Cao ∗ Department of Mathematics, Southeast University, Nanjing 210096, China Received 5 January 2005; accepted 9 March 2005 Abstract In this paper, the van der Pol equation with a time delay is considered, where the time delay is regarded as a parameter. It is found that Hopf bifurcation occurs when this delay passes through a sequence of critical value. A formula for determining the direction of the Hopf bifurcation and the stability of bifurcating periodic solutions is given by using the normal form method and center manifold theorem. © 2005 Published by Elsevier Ltd. Keywords: Van der Pol equation; Time delay; Hopf bifurcation; Periodic solutions 1. Introduction The well-known van der Pol equation, which describes the oscillations is the second-order nonlinear damped system governed by x(t)˙ = y(t) − f (x(t)), y(t)˙ =−x(t). (1.1) This model is considered as one of the most intensely studied system in nonlinear system [9,12,23] and has served as a basic model in physics, electronics, biology, neurology and ଁ This work was jointly supported by the National Natural Science Foundation of China under Grant 60373067, the 973 Program of China under Grant 2003CB317004, the Natural Science Foundation of Jiangsu Province, China under Grants BK2003053, Qing-Lan Engineering Project of Jiangsu Province, China. ∗ Corresponding author. Tel.: +86 25 83792315; fax: +86 25 83792316. E-mail address: [email protected] (J. Cao).
    [Show full text]
  • 1 Introduction 2 the Van Der Pol Oscillator
    Van der Pol Oscillator Celestial Mechanics Wesley Cao · 1 Introduction The van der Pol oscillator is a non-conservative oscillator with non-linear damping. Energy is dissipated at high amplitudes and generated at low amplitudes. As a result, there exists oscillations around a state at which energy generation and dissipation balance. The state towards which the oscillations converge is known as a limit cycle, which shall be formalized later in this paper. Balthazar van der Pol was a pioneer in the field of radio and telecommunications. While he was working at Phillips, van der Pol discovered these stable oscillations. Van der Pol himself came across the system as he was building electronic circuit models of the human heart. Due to the unique nature of the van der Pol oscillator, it has become the cornerstone for studying systems with limit cycle oscillations. In fact, the van der Pol equation has become a staple model for oscillatory processes in not only physics, but also biology, sociology and even economics. For instance, it has been used to model the electrical potential across the cell membranes of neurons in the gastric mill circuit of lobsters [5, 9]. Additionally, Fitzhugh and Nagumo used the model to describe spike generation in giant squid axons [4, 7]. The equation has also been extended to the Burridge–Knopoff model which characterizes earthquake faults with viscous friction [3]. Thus, it stands to reason that we should develop a deep understanding of the van der Pol oscillator due to its widespread applications. 2 The Van der Pol Oscillator The van der Pol oscillator is described by the equation x¨ ǫ(1 x2)x ˙ + x = 0 − − and equivalently the autonomous system, x3 x˙ = y F (x) := y ǫ x − − µ 3 − ¶ y˙ = x − It differs from the systems we have studied in that it is non-conservative.
    [Show full text]
  • Deterministic Chaos: Applications in Cardiac Electrophysiology Misha Klassen Western Washington University, [email protected]
    Occam's Razor Volume 6 (2016) Article 7 2016 Deterministic Chaos: Applications in Cardiac Electrophysiology Misha Klassen Western Washington University, [email protected] Follow this and additional works at: https://cedar.wwu.edu/orwwu Part of the Medicine and Health Sciences Commons Recommended Citation Klassen, Misha (2016) "Deterministic Chaos: Applications in Cardiac Electrophysiology," Occam's Razor: Vol. 6 , Article 7. Available at: https://cedar.wwu.edu/orwwu/vol6/iss1/7 This Research Paper is brought to you for free and open access by the Western Student Publications at Western CEDAR. It has been accepted for inclusion in Occam's Razor by an authorized editor of Western CEDAR. For more information, please contact [email protected]. Klassen: Deterministic Chaos DETERMINISTIC CHAOS APPLICATIONS IN CARDIAC ELECTROPHYSIOLOGY BY MISHA KLASSEN I. INTRODUCTION Our universe is a complex system. It is made up A system must have at least three dimensions, of many moving parts as a dynamic, multifaceted and nonlinear characteristics, in order to generate machine that works in perfect harmony to create deterministic chaos. When nonlinearity is introduced the natural world that allows us life. e modeling as a term in a deterministic model, chaos becomes of dynamical systems is the key to understanding possible. ese nonlinear dynamical systems are seen the complex workings of our universe. One such in many aspects of nature and human physiology. complexity is chaos: a condition exhibited by an is paper will discuss how the distribution of irregular or aperiodic nonlinear deterministic system. blood throughout the human body, including factors Data that is generated by a chaotic mechanism will a ecting the heart and blood vessels, demonstrate appear scattered and random, yet can be dened by chaotic behavior.
    [Show full text]
  • Dynamics of a 2D Lattice of Van Der Pol Oscillators with Nonlinear Repulsive Coupling
    Dynamics of a 2D lattice of van der Pol oscillators with nonlinear repulsive coupling I.A. Shepelev ,∗ S.S. Muni ,y T.E. Vadivasova∗ September 22, 2020 Abstract We describe spatiotemporal patterns in a network of identical van der Pol oscillators coupled in a two-dimensional geometry. In this study, we show that the system under study demonstrates a plethora of different spatiotemporal structures including chimera states when the coupling pa- rameters are varied. Spiral wave chimeras are formed in the network when the coupling strength is rather large and the coupling range is short enough. Another type of chimeras is a target wave chimera. It is shown that solitary states play a crucial role in forming an incoherence cluster of this chimera state. They can also spread within the coherence cluster. Furthermore, when the coupling range increases, the target wave chimera evolves to the regime of solitary states which are randomly distributed in space. Growing the coupling strength leads to the attraction of solitary states to a certain spatial region, while the synchronous regime is set in the other part of the system. This spatiotemporal pattern represents a soli- tary state chimera, which is firstly found in the system of continuous-time oscillators. We offer the explanation of these phenomena and describe the evolution of the regimes in detail. Introduction The study of the self-organization phenomena in complex multicomponent sys- tems in the form of oscillatory networks and ensembles is one of the most relevant arXiv:2009.09584v1 [nlin.AO] 21 Sep 2020 directions in the nonlinear dynamics and related disciplines [18, 28, 30, 4, 8].
    [Show full text]
  • Invariant Manifolds of the Bonhoeffer-Van Der Pol Oscillator
    Invariant manifolds of the Bonhoeffer-van der Pol oscillator R. Ben´ıtez1, V. J. Bol´os2 1 Dpto. Matem´aticas,Centro Universitario de Plasencia, Universidad de Extremadura. Avda. Virgen del Puerto 2. 10600, Plasencia (C´aceres),Spain. e-mail: [email protected] 2 Dpto. Matem´aticas,Facultad de Ciencias, Universidad de Extremadura. Avda. de Elvas s/n. 06071, Badajoz, Spain. e-mail: [email protected] May 2007 Abstract The stable and unstable manifolds of a saddle fixed point (SFP) of the Bonhoeffer- van der Pol oscillator are numerically studied. A correspondence between the existence of homoclinic tangencies (which are related to the creation or destruction of Smale horseshoes) and the chaos observed in the bifurcation diagram is described. It is observed that in the non-chaotic zones of the bifurcation diagram, there may or may not be Smale horseshoes, but there are no homoclinic tangencies. 1 Introduction The Bonhoeffer van der Pol oscillator (BvP) is the non-autonomous planar system 9 x3 x0 = x − − y + I(t) = 3 ; (1) y0 = c(x + a − by) ; being a, b, c real parameters, and I (t) an external forcement. We shall consider only a periodic forcement I(t) = A cos (2πt) and the specific values for the parameters a = 0:7, b = 0:8, c = 0:1. These values were considered in [1] because of their physical and biological importance (see [2]). In previous works [3], the existence of \horseshoe chaos" in BvP was studied analytically by means of the Melnikov method applied to an equivalent system, the Duffing-van der Pol oscillator (DvP).
    [Show full text]
  • 1 Van Der Pol Oscillator
    1 Van der Pol oscillator The second order non-linear autonomous differential equation d2x dx + µ x2 − 1 + x =0, µ> 0 (1) dt2 dt is called the van der Pol equation. It describes many physical systems collec- tively called van der Pol oscillators. The equation models a non-conservative system in which energy is added to and subtracted from the system, result- ing in a periodic motion called a limit cycle. The parameter mu is a positive scalar indicating the nonlinearity and the strength of the damping. The dx sign of the damping term in Eq. (1), x2 − 1 changes, depending upon dt whether |x| is larger or smaller than unity. 1.1 Numerical integration Let’s write Eq. (1) as a first order system of differential equations, dx = y, dt (2) dy 2 dx = −µ (x − 1) − x, dt dt The results of numerical integration of Eqs. (2) are presented in Figs. 1–4. Numerical integration of Eq. (2) shows that every initial condition (except x = 0,x ˙ = 0) approaches a unique periodic motion. The nature of this limit cycle is dependent on the value of µ. For small values of µ the motion is nearly sinusoidal, whereas for large values of µ it is a relaxation oscillation, meaning that it tends to resemble a series of step functions, jumping between positive and negative values twice per cycle. Numerical integration shows that the limit cycle is a closed curve en- closing the origin in the x-y phase plane. From the fact that Eqs. (2) are invariant under the transformation x → −x, y → −y, we may conclude that the curve representing the limit cycle is point symmetric about the origin.
    [Show full text]
  • Arxiv:1910.05233V1 [Physics.Comp-Ph] 11 Oct 2019 Email Address: [email protected] (Artem Chashchin)
    Predicting dynamical system evolution with residual neural networks Artem Chashchina,b,∗, Mikhail Botcheva, Ivan Oseledetsb,c, George Ovchinnikovb aKeldysh Institute of Applied Mathematics of the Russian Academy of Sciences, Moscow, Russia bSkolkovo Institute of Science and Technology, Moscow, Russia cMarchuk Institute of Numerical Mathematics of the Russian Academy of Sciences, Moscow, Russia Abstract Forecasting time series and time-dependent data is a common problem in many applications. One typical example is solving ordinary differential equation (ODE) systemsx _ = F (x). Oftentimes the right hand side function F (x) is not known explicitly and the ODE system is described by solution samples taken at some time points. Hence, ODE solvers cannot be used. In this paper, a data- driven approach to learning the evolution of dynamical systems is considered. We show how by training neural networks with ResNet-like architecture on the solution samples, models can be developed to predict the ODE system solution further in time. By evaluating the proposed approaches on three test ODE systems, we demonstrate that the neural network models are able to reproduce the main dynamics of the systems qualitatively well. Moreover, the predicted solution remains stable for much longer times than for other currently known models. Keywords: dynamical systems, residual networks, deep learning ∗Corresponding author arXiv:1910.05233v1 [physics.comp-ph] 11 Oct 2019 Email address: [email protected] (Artem Chashchin) Preprint submitted to Journal of Computational Physics October 14, 2019 1. Introduction Neural network techniques are becoming an important tool for analyzing time-dependent data sets and multivariate time series. One typical problem is to reconstruct solution of an ODE (ordinary differential equation) system x_ = F (x) by learning the right hand side function F (x) with a suitable neural network.
    [Show full text]
  • 8 Example 1: the Van Der Pol Oscillator (Strogatz Chapter 7)
    Dynamical systems 2018 [email protected] 8 Example 1: The van der Pol oscillator (Strogatz Chapter 7) So far we have seen some different possibilities of what can happen in two-dimensional systems (local and global attractors and bifurcations) using mainly constructed examples. In this and the next lectures we consider two examples with real-world applications. 8.1 Self-sustained oscillations Self-sustained oscillations are frequent in nature and in technology, some examples being stick-slip oscillations, unwanted mechanical vi- brations, and oscillators in biology. Usually a system with self-sustained oscillations has a feedback mechanism such that small-amplitude os- cillations grow in size. The small oscillations are frequently modeled using an oscillator with negative damping 2 x¨ − γx_ + !0x = 0 : The system for x and y =x _ has an unstable spiral at the origin, blow- ing up small-scale oscillations. As oscillations grow, non-linear terms may form a stable limit cycle and the system shows self-sustained oscillations. One frequently used model is the van der Pol oscillator: x¨ + µ(x2 − 1) x_ + x = 0 (1) | {z } f(x) Nonlinear damping coefficient f(x) damps large oscillations (friction when jxj > 1) and amplifies small oscillations (forcing when jxj < 1) ) We expect self-sustained oscillations to be possible. Indeed the corresponding dynamical system x_ = y y_ = −x − µ(x2 − 1)y 0 p shows ap stable limit cycle if µ > 0 (after a rescaling x = x = µ and y = y0= µ, the system has a supercritical Hopf bifurcation): 1 Dynamical systems 2018 [email protected] Period time and shape of the cycle depends on µ.
    [Show full text]